{ "cells": [ { "cell_type": "markdown", "id": "5637f725", "metadata": { "tags": [ "papermill-error-cell-tag" ] }, "source": [ "An Exception was encountered at 'In [10]'." ] }, { "cell_type": "markdown", "execution_count": null, "id": "5ed63800", "metadata": { "papermill": { "duration": 0.003872, "end_time": "2026-08-04T14:43:20.316275+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.312403+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "### L shaped antenna simulation.\n", "\n", "In this notebook we will generate the mesh of an L shaped antenna and generate a json for a transient\n", "simulation." ] }, { "cell_type": "code", "execution_count": 1, "id": "9437354e", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:20.323453Z", "iopub.status.busy": "2026-08-04T14:43:20.323248Z", "iopub.status.idle": "2026-08-04T14:43:20.835834Z", "shell.execute_reply": "2026-08-04T14:43:20.835158Z" }, "papermill": { "duration": 0.517356, "end_time": "2026-08-04T14:43:20.836730+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.319374+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "import gmsh\n", "\n", "from palacetoolkit.simulation import generate_palace_config_from_entities\n", "from palacetoolkit.viz import view_mesh\n", "from palacetoolkit.mesh import (\n", " Entity, \n", " run_entity_pipeline, \n", " generate_3d_mesh, \n", " create_graded_mesh\n", ")" ] }, { "cell_type": "markdown", "execution_count": null, "id": "1d956d7d", "metadata": { "papermill": { "duration": 0.003204, "end_time": "2026-08-04T14:43:20.843712+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.840508+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "\n", "### Parameters:\n", "- h : Patch height along z-axis, specified as a scalar in meters. \n", "- l1 : Ground plane length along x-axis, specified as a scalar in meters\n", "- w1 : Ground plane width along y-axis, specified as a scalar in meters\n", "- w3 : Strip line width along y-axis, specified as a scalar in meters.\n", "- air_height : Air box height along z-axis, specified as a scalar in meters. \n", "- air_margin : Air box margin along x and y axes, specified as a scalar in meters.\n", "- freq : Simulation frequency in GHz, specified as a scalar.\n", "- filename : Output mesh filename, specified as a string." ] }, { "cell_type": "code", "execution_count": 2, "id": "4049c4db", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:20.851194Z", "iopub.status.busy": "2026-08-04T14:43:20.850955Z", "iopub.status.idle": "2026-08-04T14:43:20.854325Z", "shell.execute_reply": "2026-08-04T14:43:20.853688Z" }, "papermill": { "duration": 0.008113, "end_time": "2026-08-04T14:43:20.855047+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.846934+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "l1: float = 0.06\n", "w1: float = 0.06\n", "w3: float = 0.002\n", "h: float = 0.0013\n", "air_height: float = 0.025 \n", "air_margin: float = 0.025 \n", "freq: float = 3.3\n", "mesh_file: str = \"l_antenna.msh\"\n", "\n", "\n", "eps_r: float = 2.2\n", "loss_tan: float = 0.0009\n", "\n", "wavelength = 3e8 / (freq * 1e9)\n", "mesh_size = wavelength / 15" ] }, { "cell_type": "markdown", "execution_count": null, "id": "6d496609", "metadata": { "papermill": { "duration": 0.003153, "end_time": "2026-08-04T14:43:20.861473+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.858320+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "### Initialize the model" ] }, { "cell_type": "code", "execution_count": 3, "id": "e6a08089", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:20.887391Z", "iopub.status.busy": "2026-08-04T14:43:20.887231Z", "iopub.status.idle": "2026-08-04T14:43:20.890758Z", "shell.execute_reply": "2026-08-04T14:43:20.890073Z" }, "papermill": { "duration": 0.0081, "end_time": "2026-08-04T14:43:20.891274+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.883174+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "gmsh.initialize()\n", "gmsh.model.add(\"patch_antenna\")\n", "kernel = gmsh.model.occ" ] }, { "cell_type": "markdown", "execution_count": null, "id": "783686ab", "metadata": { "papermill": { "duration": 0.003314, "end_time": "2026-08-04T14:43:20.897894+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.894580+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "### Geometry Construction\n" ] }, { "cell_type": "code", "execution_count": 4, "id": "474cc986", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:20.905220Z", "iopub.status.busy": "2026-08-04T14:43:20.905067Z", "iopub.status.idle": "2026-08-04T14:43:20.916688Z", "shell.execute_reply": "2026-08-04T14:43:20.916025Z" }, "papermill": { "duration": 0.016114, "end_time": "2026-08-04T14:43:20.917283+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.901169+00:00", "status": "completed" }, "tags": [] }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Info : [ 0%] Union \r", "Info : [ 10%] Union \r", "Info : [ 20%] Union - Performing Vertex-Face intersection \r", "Info : [ 30%] Union \r", "Info : [ 40%] Union \r", "Info : [ 50%] Union \r", "Info : [ 60%] Union \r", "Info : [ 70%] Union - Filling splits of vertices \r", "Info : [ 80%] Union - Splitting faces \r", " \r", "Info : Cannot bind existing OpenCASCADE surface 9 to second tag 10\n", "Info : Could not preserve tag of 2D object 10 (->9)\n" ] } ], "source": [ "total_xmin = -l1/2 - air_margin\n", "total_xmax = l1/2 + air_margin\n", "total_ymin = -w1/2 - air_margin\n", "total_ymax = w1/2 + air_margin\n", "total_zmax = h + air_height\n", "\n", "\n", "# 1. Create volumes\n", "substrate = kernel.addBox(-l1/2, -w1/2, 0, l1, w1, h)\n", "airsphere_radius = max(abs(total_xmin), abs(total_xmax), abs(total_ymin), abs(total_ymax), total_zmax)\n", "air_sphere = kernel.addSphere(0.0, 0.0, 0.0, airsphere_radius)\n", "kernel.synchronize()\n", "\n", "# 2. Create 2D surfaces (ground, patch, ports)\n", "ground_plane = kernel.addRectangle(-l1/2, -w1/2, 0, l1, w1)\n", "\n", "strip_length_x = l1/2\n", "strip_length_y = w1/2 + w3/2\n", "\n", "feed_line_x = kernel.addRectangle(-l1/2, -w3/2, h, strip_length_x, w3)\n", "feed_line_y = kernel.addRectangle(0, -w3/2, h, w3, strip_length_y)\n", "\n", "top_conductor, top_map = kernel.fuse(\n", " [(2, feed_line_x)], [(2, feed_line_y)],\n", " removeObject=True, removeTool=True\n", ")\n", "kernel.synchronize()\n", "\n", "# Lumped ports - build directly in-plane, no rotation\n", "# Port 1: at x = -l1/2, vertical face\n", "p1 = kernel.addPoint(-l1/2, -w3/2, 0)\n", "p2 = kernel.addPoint(-l1/2, w3/2, 0)\n", "p3 = kernel.addPoint(-l1/2, w3/2, h)\n", "p4 = kernel.addPoint(-l1/2, -w3/2, h)\n", "\n", "lp1_a = kernel.addLine(p1, p2)\n", "lp1_b = kernel.addLine(p2, p3)\n", "lp1_c = kernel.addLine(p3, p4)\n", "lp1_d = kernel.addLine(p4, p1)\n", "loop1 = kernel.addCurveLoop([lp1_a, lp1_b, lp1_c, lp1_d])\n", "lumped_port_1 = kernel.addPlaneSurface([loop1])\n", "kernel.synchronize()\n", "\n", "# Port 2: at y = w1/2, vertical face\n", "p5 = kernel.addPoint(0, w1/2, 0)\n", "p6 = kernel.addPoint(w3, w1/2, 0)\n", "p7 = kernel.addPoint(w3, w1/2, h)\n", "p8 = kernel.addPoint(0, w1/2, h)\n", "\n", "lp2_a = kernel.addLine(p5, p6)\n", "lp2_b = kernel.addLine(p6, p7)\n", "lp2_c = kernel.addLine(p7, p8)\n", "lp2_d = kernel.addLine(p8, p5)\n", "loop2 = kernel.addCurveLoop([lp2_a, lp2_b, lp2_c, lp2_d])\n", "lumped_port_2 = kernel.addPlaneSurface([loop2])\n", "kernel.synchronize()\n", "\n", "# Define the entities which will be the physical groups.\n", "entities = [\n", " Entity(\"substrate\", dim=3, btype=\"dielectric\", mesh_order=1, tags=[substrate], loss_tan=loss_tan, eps_r=eps_r, mu_r=1.0),\n", " Entity(\"air_sphere\", dim=3, btype=\"dielectric\", mesh_order=2, tags=[air_sphere], loss_tan=0.0, eps_r=1.0, mu_r=1.0),\n", " Entity(\"top_conductor\", dim=2, btype=\"pec\", mesh_order=1, tags=[top_conductor[0][1]]),\n", " Entity(\"ground_plane\", dim=2, btype=\"pec\", mesh_order=1, tags=[ground_plane]),\n", " Entity(\"lumped_port_1\", dim=2, btype=\"lumped_port\", mesh_order=0, tags=[lumped_port_1], R=50.0, direction=\"+Z\", excitation=True),\n", " Entity(\"lumped_port_2\", dim=2, btype=\"lumped_port\", mesh_order=0, tags=[lumped_port_2], R=50.0, direction=\"+Z\", excitation=False),\n", "]\n" ] }, { "cell_type": "code", "execution_count": 5, "id": "ecf93353", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:20.924305Z", "iopub.status.busy": "2026-08-04T14:43:20.924165Z", "iopub.status.idle": "2026-08-04T14:43:27.777235Z", "shell.execute_reply": "2026-08-04T14:43:27.776551Z" }, "papermill": { "duration": 6.85782, "end_time": "2026-08-04T14:43:27.778328+00:00", "exception": false, "start_time": "2026-08-04T14:43:20.920508+00:00", "status": "completed" }, "tags": [] }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ " Physical group 'substrate' (dim=3): pg=1, tags=[1]\n", " Physical group 'air_sphere' (dim=3): pg=2, tags=[2]\n", " Physical group 'top_conductor' (dim=2): pg=3, tags=[9]\n", " Physical group 'ground_plane' (dim=2): pg=4, tags=[8]\n", " Physical group 'lumped_port_1' (dim=2): pg=5, tags=[10]\n", " Physical group 'lumped_port_2' (dim=2): pg=6, tags=[11]\n", " Physical group 'air_sphere__substrate' (dim=2): pg=7, tags=[12, 13, 14, 15, 16, 17, 18, 19]\n", " Physical group 'air_sphere__None' (dim=2): pg=8, tags=[20]\n", " ignoring 3 curves from {'air_sphere__None'}\n", " global: 28 curves, SizeMin=0.0009\n", " ppw_near=100 ppw_far=15\n", " SizeMax=0.0061 transition=0.0227\n", " local: dimtag=(2, 11), ppw=100, SizeMin=0.0009\n", " local: dimtag=(2, 10), ppw=100, SizeMin=0.0009\n" ] } ], "source": [ "pg_map = run_entity_pipeline(entities)\n", "\n", "lumped_port_1 = entities[-1].dimtags[0]\n", "lumped_port_2 = entities[-2].dimtags[0]\n", "\n", "# Refine near the top conductor and also locally refine the ports.\n", "create_graded_mesh( wavelength, \n", " ppw_near=100, \n", " ppw_far=15, \n", " set_as_background=True,\n", " local_refinements = {lumped_port_1: 100, lumped_port_2 : 100})\n", "\n", "mesh_sizes = {\n", " \"substrate\": wavelength / 12,\n", " \"air_sphere\": wavelength / 4,\n", " \"lumped_port_1\": wavelength / 18,\n", " \"lumped_port_2\": wavelength / 18,\n", " \"top_conductor\": wavelength /10\n", "}\n", "\n", "generate_3d_mesh(entities, mesh_sizes, mesh_file, optimize=True, verbose=False)\n", "gmsh.finalize()" ] }, { "cell_type": "code", "execution_count": 6, "id": "f2fc1ec1", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:27.786083Z", "iopub.status.busy": "2026-08-04T14:43:27.785924Z", "iopub.status.idle": "2026-08-04T14:43:28.740801Z", "shell.execute_reply": "2026-08-04T14:43:28.739988Z" }, "papermill": { "duration": 0.959582, "end_time": "2026-08-04T14:43:28.741454+00:00", "exception": false, "start_time": "2026-08-04T14:43:27.781872+00:00", "status": "completed" }, "tags": [] }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Loading mesh file: l_antenna.msh\n", "Groups to render transparent: air_sphere__None\n", "\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ "Mesh loaded successfully with 2 cell blocks\n", "Found 10310 triangles total\n", "Physical group tags in mesh: {3: 'top_conductor', 4: 'ground_plane', 5: 'lumped_port_1', 6: 'lumped_port_2', 7: 'air_sphere__substrate', 8: 'air_sphere__None'}\n" ] }, { "data": { "image/png": "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", "text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "view_mesh(mesh_file, transparent_groups= \"air_sphere__None\")" ] }, { "cell_type": "markdown", "execution_count": null, "id": "cde1861e", "metadata": { "papermill": { "duration": 0.003632, "end_time": "2026-08-04T14:43:28.749119+00:00", "exception": false, "start_time": "2026-08-04T14:43:28.745487+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "### Simulation Configuration\n", "We define the key parameters for the electromagnetic simulation here. These settings control the frequency sweep range, material properties (dielectric constant and loss tangent for the substrate), and solver-specific configurations like port impedance and mesh order.\n", "\n", "- output_file : output filename for the configuration JSON file\n", "- freq : frequency for the simulation (GHz) \n", "- eps_r: relative permittivity of the substrate\n", "- loss_tan: loss tangent of the substrate\n", "- port_impedance: characteristic impedance of the lumped port (Ohms)\n", "- solver_order: order of the finite element basis functions for the simulation (e.g., 1 for linear, 2 for quadratic)" ] }, { "cell_type": "code", "execution_count": 7, "id": "8a378602", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:28.757510Z", "iopub.status.busy": "2026-08-04T14:43:28.757335Z", "iopub.status.idle": "2026-08-04T14:43:28.760926Z", "shell.execute_reply": "2026-08-04T14:43:28.760053Z" }, "papermill": { "duration": 0.008587, "end_time": "2026-08-04T14:43:28.761443+00:00", "exception": false, "start_time": "2026-08-04T14:43:28.752856+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "output_file_transient: str = \"l_antenna_transient.json\"\n", "output_file_driven: str = \"l_antenna_driven.json\"\n", "\n", "freq: float = 3.64\n", "eps_r: float = 2.2\n", "loss_tan: float = 0.0009\n", "port_impedance: float = 50.0\n", "solver_order: int = 2\n", "\n", "freq_min = 3.3\n", "freq_max = 3.8\n", "freq_step = 0.01\n", "\n", "import numpy as np\n", "eps_0 = 8.8541878128e-12\n", "sigma = 2 * np.pi * freq * eps_0 * eps_r * loss_tan" ] }, { "cell_type": "markdown", "execution_count": null, "id": "a0161718", "metadata": { "papermill": { "duration": 0.004395, "end_time": "2026-08-04T14:43:28.802386+00:00", "exception": false, "start_time": "2026-08-04T14:43:28.797991+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "### Generating the Palace Configuration File\n", "Finally, we assemble the simulation parameters into two JSON configuration. One for a transient simulation and one for a driven where we check the s-parameters." ] }, { "cell_type": "code", "execution_count": 8, "id": "abf062be", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:28.812276Z", "iopub.status.busy": "2026-08-04T14:43:28.812063Z", "iopub.status.idle": "2026-08-04T14:43:28.816913Z", "shell.execute_reply": "2026-08-04T14:43:28.816237Z" }, "papermill": { "duration": 0.010445, "end_time": "2026-08-04T14:43:28.817437+00:00", "exception": false, "start_time": "2026-08-04T14:43:28.806992+00:00", "status": "completed" }, "tags": [] }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Palace config written to l_antenna_transient.json\n", "Palace config written to l_antenna_driven.json\n" ] } ], "source": [ "config_transient = generate_palace_config_from_entities(\n", " entity_defs= [e.to_dict() for e in entities],\n", " pg_map=pg_map,\n", " mesh_file=mesh_file,\n", " output_file=output_file_transient,\n", " sim_type=\"transient\",\n", " excitation_freq=freq,\n", " excitation_width=0.05,\n", " max_time=0.5,\n", " time_step=0.005,\n", " save_step=2,\n", ")\n", "\n", "config_driven = generate_palace_config_from_entities(\n", " entity_defs= [e.to_dict() for e in entities],\n", " pg_map=pg_map,\n", " mesh_file=mesh_file,\n", " output_file=output_file_driven,\n", " sim_type=\"driven\",\n", " L0=1.0,\n", " solver_order=2,\n", " absorbing_order=1,\n", " farfield=False, \n", " freq_min=3.3,\n", " freq_max=3.8,\n", " freq_step=0.01,\n", " linear_maxits=300, \n", ")" ] }, { "cell_type": "markdown", "execution_count": null, "id": "0e13ce9f", "metadata": { "papermill": { "duration": 0.004057, "end_time": "2026-08-04T14:43:28.825549+00:00", "exception": false, "start_time": "2026-08-04T14:43:28.821492+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "### Running PALACE" ] }, { "cell_type": "code", "execution_count": 9, "id": "9554847a", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T14:43:28.834836Z", "iopub.status.busy": "2026-08-04T14:43:28.834642Z", "iopub.status.idle": "2026-08-04T15:58:21.636421Z", "shell.execute_reply": "2026-08-04T15:58:21.635630Z" }, "papermill": { "duration": 4492.813587, "end_time": "2026-08-04T15:58:21.643504+00:00", "exception": false, "start_time": "2026-08-04T14:43:28.829917+00:00", "status": "completed" }, "tags": [] }, "outputs": [ { "data": { "text/html": [ "
Palace simulation output
  Running: /home/runner/.cache/palacetoolkit/runtime/palace-cpu-v0.17.0/bin/palace --serial /home/runner/work/PalaceToolkit/PalaceToolkit/docs/examples/l_antenna_transient.json\n",
       ">> /home/runner/.cache/palacetoolkit/runtime/palace-cpu-v0.17.0/bin/palace-x86_64.bin /home/runner/work/PalaceToolkit/PalaceToolkit/docs/examples/l_antenna_transient.json\n",
       "\n",
       "_____________     _______\n",
       "_____   __   \\____ __   /____ ____________\n",
       "____   /_/  /  __ ` /  /  __ ` /  ___/  _ \\\n",
       "___   _____/  /_/  /  /  /_/  /  /__/  ___/\n",
       "  /__/     \\___,__/__/\\___,__/\\_____\\_____/\n",
       "\n",
       "Git changeset ID: v0.17.0-272-gb22f654ab\n",
       "Running with 1 MPI process, 1 OpenMP thread\n",
       "Device configuration: omp,cpu\n",
       "Memory configuration: host-std\n",
       "libCEED backend: /cpu/self/xsmm/blocked\n",
       "\n",
       "Added 1443 duplicate vertices for interior boundaries in the mesh\n",
       "Added 3286 duplicate boundary elements for interior boundaries in the mesh\n",
       "\n",
       "Characteristic length and time scales:\n",
       " Lc = 1.100e-04 m, tc = 3.669e-04 ns\n",
       "Finished partitioning mesh into 1 subdomain\n",
       "\n",
       "Mesh curvature order: 1\n",
       "Mesh bounding box:\n",
       " (Xmin, Ymin, Zmin) = (-5.497e-05, -5.500e-05, -5.500e-05) m\n",
       " (Xmax, Ymax, Zmax) = (+5.492e-05, +5.491e-05, +5.500e-05) m\n",
       "\n",
       "Parallel Mesh Stats:\n",
       "\n",
       "                minimum     average     maximum       total\n",
       " vertices         16196       16196       16196       16196\n",
       " edges           103526      103526      103526      103526\n",
       " faces           169866      169866      169866      169866\n",
       " elements         82533       82533       82533       82533\n",
       " neighbors            0           0           0\n",
       "\n",
       "            minimum     maximum\n",
       " h       0.00474058   0.0966723\n",
       " kappa      1.05585     7.38466\n",
       "\n",
       "Estimated current per-rank memory usage is: Min. 107.5M, Max. 107.5M, Avg. 107.5M, Total 107.5M\n",
       "Estimated current per-node memory usage is: Min. 107.5M, Max. 107.5M, Avg. 107.5M, Total 107.5M\n",
       "\n",
       "Configuring Robin absorbing BC (order 1) at attributes:\n",
       " 8\n",
       "\n",
       "Configuring Robin impedance BC for lumped ports at attributes:\n",
       " 5: Rs = 7.692e+01 Ω/sq, n = (-1.0,+0.0,+0.0)\n",
       " 6: Rs = 7.692e+01 Ω/sq, n = (+0.0,+1.0,+0.0)\n",
       "\n",
       "Configuring lumped port circuit properties:\n",
       " Index = 1: R = 5.000e+01 Ω\n",
       " Index = 2: R = 5.000e+01 Ω\n",
       "\n",
       "Configuring lumped port excitation source term at attributes:\n",
       " 5: Index = 1\n",
       "\n",
       "Configuring Dirichlet PEC BC at attributes:\n",
       " 3-4\n",
       "\n",
       "Assembling system matrices, number of global unknowns:\n",
       " H1 (p = 2): 119722, ND (p = 2): 546784, RT (p = 2): 757197\n",
       " Operator assembly level: Partial\n",
       " Mesh geometries:\n",
       "  Tetrahedron: P = 20, Q = 14 (quadrature order = 4)\n",
       "\n",
       "Computing transient response for:\n",
       "Excitation with index 1 has contributions from:\n",
       " Lumped port  1\n",
       "\n",
       "It 0/100: t = 0.000000e+00 ns (elapsed time = 4.10e-07 s)\n",
       "\n",
       " Sol. ||E|| = 0.000000e+00, ||B|| = 0.000000e+00\n",
       " Field energy E (0.000e+00 J) + H (0.000e+00 J) = 0.000e+00 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 1\n",
       " Updating solution error estimates\n",
       "\n",
       "It 1/100: t = 5.000000e-03 ns (elapsed time = 1.03e+01 s)\n",
       "\n",
       "Assembling multigrid hierarchy:\n",
       " Level 0 (p = 1): 103526 unknowns\n",
       " Level 1 (p = 2): 546784 unknowns\n",
       " Level 0 (auxiliary) (p = 1): 16196 unknowns\n",
       " Level 1 (auxiliary) (p = 2): 119722 unknowns\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.269615e-07\n",
       "  1 KSP residual norm ||r||_B = 9.638581e-08\n",
       "  2 KSP residual norm ||r||_B = 9.090338e-08\n",
       "  3 KSP residual norm ||r||_B = 1.059638e-07\n",
       "  4 KSP residual norm ||r||_B = 1.034920e-07\n",
       "  5 KSP residual norm ||r||_B = 1.117599e-07\n",
       "  6 KSP residual norm ||r||_B = 1.270557e-07\n",
       "  7 KSP residual norm ||r||_B = 1.577894e-07\n",
       "  8 KSP residual norm ||r||_B = 1.744215e-07\n",
       "  9 KSP residual norm ||r||_B = 1.860081e-07\n",
       " 10 KSP residual norm ||r||_B = 1.739801e-07\n",
       " 11 KSP residual norm ||r||_B = 1.199749e-07\n",
       " 12 KSP residual norm ||r||_B = 5.284112e-08\n",
       " 13 KSP residual norm ||r||_B = 1.724502e-08\n",
       " 14 KSP residual norm ||r||_B = 6.041985e-09\n",
       " 15 KSP residual norm ||r||_B = 1.954417e-09\n",
       " 16 KSP residual norm ||r||_B = 5.965344e-10\n",
       " 17 KSP residual norm ||r||_B = 1.753302e-10\n",
       " 18 KSP residual norm ||r||_B = 4.116981e-11\n",
       " 19 KSP residual norm ||r||_B = 9.040539e-12\n",
       " 20 KSP residual norm ||r||_B = 1.971564e-12\n",
       " 21 KSP residual norm ||r||_B = 4.175612e-13\n",
       " 22 KSP residual norm ||r||_B = 8.445354e-14\n",
       " 23 KSP residual norm ||r||_B = 1.724028e-14\n",
       " 24 KSP residual norm ||r||_B = 4.009776e-15\n",
       " 25 KSP residual norm ||r||_B = 9.299870e-16\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.727e-01)\n",
       " Sol. ||E|| = 6.207456e-04, ||B|| = 1.184226e-05\n",
       " Field energy E (4.679e-23 J) + H (8.907e-23 J) = 1.359e-22 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 2/100: t = 1.000000e-02 ns (elapsed time = 6.79e+01 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 3.218285e-07\n",
       "  1 KSP residual norm ||r||_B = 2.402797e-07\n",
       "  2 KSP residual norm ||r||_B = 2.136394e-07\n",
       "  3 KSP residual norm ||r||_B = 2.067418e-07\n",
       "  4 KSP residual norm ||r||_B = 1.534972e-07\n",
       "  5 KSP residual norm ||r||_B = 1.107430e-07\n",
       "  6 KSP residual norm ||r||_B = 1.037793e-07\n",
       "  7 KSP residual norm ||r||_B = 1.630805e-07\n",
       "  8 KSP residual norm ||r||_B = 2.904015e-07\n",
       "  9 KSP residual norm ||r||_B = 3.066860e-07\n",
       " 10 KSP residual norm ||r||_B = 2.401787e-07\n",
       " 11 KSP residual norm ||r||_B = 2.028163e-07\n",
       " 12 KSP residual norm ||r||_B = 1.123193e-07\n",
       " 13 KSP residual norm ||r||_B = 3.391701e-08\n",
       " 14 KSP residual norm ||r||_B = 1.089747e-08\n",
       " 15 KSP residual norm ||r||_B = 3.959792e-09\n",
       " 16 KSP residual norm ||r||_B = 1.283984e-09\n",
       " 17 KSP residual norm ||r||_B = 4.052230e-10\n",
       " 18 KSP residual norm ||r||_B = 1.028321e-10\n",
       " 19 KSP residual norm ||r||_B = 2.288850e-11\n",
       " 20 KSP residual norm ||r||_B = 4.986390e-12\n",
       " 21 KSP residual norm ||r||_B = 1.071089e-12\n",
       " 22 KSP residual norm ||r||_B = 2.178071e-13\n",
       " 23 KSP residual norm ||r||_B = 4.397948e-14\n",
       " 24 KSP residual norm ||r||_B = 1.019627e-14\n",
       " 25 KSP residual norm ||r||_B = 2.364753e-15\n",
       " 26 KSP residual norm ||r||_B = 4.796732e-16\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.652e-01)\n",
       " Sol. ||E|| = 1.618930e-03, ||B|| = 3.176163e-05\n",
       " Field energy E (3.184e-22 J) + H (6.408e-22 J) = 9.591e-22 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 3\n",
       " Updating solution error estimates\n",
       "\n",
       "It 3/100: t = 1.500000e-02 ns (elapsed time = 1.19e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 5.550643e-07\n",
       "  1 KSP residual norm ||r||_B = 4.167723e-07\n",
       "  2 KSP residual norm ||r||_B = 3.653085e-07\n",
       "  3 KSP residual norm ||r||_B = 3.300887e-07\n",
       "  4 KSP residual norm ||r||_B = 2.239714e-07\n",
       "  5 KSP residual norm ||r||_B = 1.325556e-07\n",
       "  6 KSP residual norm ||r||_B = 9.689586e-08\n",
       "  7 KSP residual norm ||r||_B = 1.325084e-07\n",
       "  8 KSP residual norm ||r||_B = 2.815588e-07\n",
       "  9 KSP residual norm ||r||_B = 4.042339e-07\n",
       " 10 KSP residual norm ||r||_B = 2.660841e-07\n",
       " 11 KSP residual norm ||r||_B = 1.781330e-07\n",
       " 12 KSP residual norm ||r||_B = 1.408980e-07\n",
       " 13 KSP residual norm ||r||_B = 5.128220e-08\n",
       " 14 KSP residual norm ||r||_B = 1.474511e-08\n",
       " 15 KSP residual norm ||r||_B = 5.185868e-09\n",
       " 16 KSP residual norm ||r||_B = 1.763136e-09\n",
       " 17 KSP residual norm ||r||_B = 6.063396e-10\n",
       " 18 KSP residual norm ||r||_B = 1.697828e-10\n",
       " 19 KSP residual norm ||r||_B = 3.921862e-11\n",
       " 20 KSP residual norm ||r||_B = 8.518479e-12\n",
       " 21 KSP residual norm ||r||_B = 1.818476e-12\n",
       " 22 KSP residual norm ||r||_B = 3.741248e-13\n",
       " 23 KSP residual norm ||r||_B = 7.680840e-14\n",
       " 24 KSP residual norm ||r||_B = 1.762443e-14\n",
       " 25 KSP residual norm ||r||_B = 4.008346e-15\n",
       " 26 KSP residual norm ||r||_B = 8.283037e-16\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.660e-01)\n",
       " Sol. ||E|| = 3.065937e-03, ||B|| = 6.003959e-05\n",
       " Field energy E (1.142e-21 J) + H (2.290e-21 J) = 3.431e-21 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 4/100: t = 2.000000e-02 ns (elapsed time = 1.58e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.465293e-07\n",
       "  1 KSP residual norm ||r||_B = 5.646997e-07\n",
       "  2 KSP residual norm ||r||_B = 4.926416e-07\n",
       "  3 KSP residual norm ||r||_B = 4.282033e-07\n",
       "  4 KSP residual norm ||r||_B = 2.767784e-07\n",
       "  5 KSP residual norm ||r||_B = 1.423500e-07\n",
       "  6 KSP residual norm ||r||_B = 7.627427e-08\n",
       "  7 KSP residual norm ||r||_B = 7.226881e-08\n",
       "  8 KSP residual norm ||r||_B = 1.422638e-07\n",
       "  9 KSP residual norm ||r||_B = 3.093015e-07\n",
       " 10 KSP residual norm ||r||_B = 2.686064e-07\n",
       " 11 KSP residual norm ||r||_B = 1.020847e-07\n",
       " 12 KSP residual norm ||r||_B = 6.485175e-08\n",
       " 13 KSP residual norm ||r||_B = 4.802184e-08\n",
       " 14 KSP residual norm ||r||_B = 1.634871e-08\n",
       " 15 KSP residual norm ||r||_B = 5.392252e-09\n",
       " 16 KSP residual norm ||r||_B = 1.768094e-09\n",
       " 17 KSP residual norm ||r||_B = 6.475582e-10\n",
       " 18 KSP residual norm ||r||_B = 2.088451e-10\n",
       " 19 KSP residual norm ||r||_B = 5.169738e-11\n",
       " 20 KSP residual norm ||r||_B = 1.132769e-11\n",
       " 21 KSP residual norm ||r||_B = 2.409609e-12\n",
       " 22 KSP residual norm ||r||_B = 4.989038e-13\n",
       " 23 KSP residual norm ||r||_B = 1.035176e-13\n",
       " 24 KSP residual norm ||r||_B = 2.363000e-14\n",
       " 25 KSP residual norm ||r||_B = 5.315390e-15\n",
       " 26 KSP residual norm ||r||_B = 1.108101e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.684e-01)\n",
       " Sol. ||E|| = 5.219159e-03, ||B|| = 1.025881e-04\n",
       " Field energy E (3.309e-21 J) + H (6.685e-21 J) = 9.993e-21 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 5\n",
       " Updating solution error estimates\n",
       "\n",
       "It 5/100: t = 2.500000e-02 ns (elapsed time = 2.08e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.322281e-07\n",
       "  1 KSP residual norm ||r||_B = 6.983330e-07\n",
       "  2 KSP residual norm ||r||_B = 6.074601e-07\n",
       "  3 KSP residual norm ||r||_B = 5.309389e-07\n",
       "  4 KSP residual norm ||r||_B = 3.427587e-07\n",
       "  5 KSP residual norm ||r||_B = 1.780060e-07\n",
       "  6 KSP residual norm ||r||_B = 9.522359e-08\n",
       "  7 KSP residual norm ||r||_B = 8.927059e-08\n",
       "  8 KSP residual norm ||r||_B = 1.700808e-07\n",
       "  9 KSP residual norm ||r||_B = 3.429408e-07\n",
       " 10 KSP residual norm ||r||_B = 3.194525e-07\n",
       " 11 KSP residual norm ||r||_B = 1.972268e-07\n",
       " 12 KSP residual norm ||r||_B = 1.749048e-07\n",
       " 13 KSP residual norm ||r||_B = 8.065602e-08\n",
       " 14 KSP residual norm ||r||_B = 2.356404e-08\n",
       " 15 KSP residual norm ||r||_B = 8.230508e-09\n",
       " 16 KSP residual norm ||r||_B = 2.805624e-09\n",
       " 17 KSP residual norm ||r||_B = 9.747424e-10\n",
       " 18 KSP residual norm ||r||_B = 2.799007e-10\n",
       " 19 KSP residual norm ||r||_B = 6.554532e-11\n",
       " 20 KSP residual norm ||r||_B = 1.424816e-11\n",
       " 21 KSP residual norm ||r||_B = 3.036145e-12\n",
       " 22 KSP residual norm ||r||_B = 6.268577e-13\n",
       " 23 KSP residual norm ||r||_B = 1.292552e-13\n",
       " 24 KSP residual norm ||r||_B = 2.961630e-14\n",
       " 25 KSP residual norm ||r||_B = 6.705946e-15\n",
       " 26 KSP residual norm ||r||_B = 1.390290e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.675e-01)\n",
       " Sol. ||E|| = 8.236126e-03, ||B|| = 1.619415e-04\n",
       " Field energy E (8.239e-21 J) + H (1.666e-20 J) = 2.490e-20 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 6/100: t = 3.000000e-02 ns (elapsed time = 2.50e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.077389e-06\n",
       "  1 KSP residual norm ||r||_B = 8.068709e-07\n",
       "  2 KSP residual norm ||r||_B = 7.012312e-07\n",
       "  3 KSP residual norm ||r||_B = 6.060294e-07\n",
       "  4 KSP residual norm ||r||_B = 3.846205e-07\n",
       "  5 KSP residual norm ||r||_B = 1.897402e-07\n",
       "  6 KSP residual norm ||r||_B = 8.393093e-08\n",
       "  7 KSP residual norm ||r||_B = 5.247293e-08\n",
       "  8 KSP residual norm ||r||_B = 7.290549e-08\n",
       "  9 KSP residual norm ||r||_B = 1.598538e-07\n",
       " 10 KSP residual norm ||r||_B = 2.278531e-07\n",
       " 11 KSP residual norm ||r||_B = 1.584861e-07\n",
       " 12 KSP residual norm ||r||_B = 1.532520e-07\n",
       " 13 KSP residual norm ||r||_B = 8.762971e-08\n",
       " 14 KSP residual norm ||r||_B = 2.663719e-08\n",
       " 15 KSP residual norm ||r||_B = 9.340676e-09\n",
       " 16 KSP residual norm ||r||_B = 3.190482e-09\n",
       " 17 KSP residual norm ||r||_B = 1.109090e-09\n",
       " 18 KSP residual norm ||r||_B = 3.209563e-10\n",
       " 19 KSP residual norm ||r||_B = 7.557774e-11\n",
       " 20 KSP residual norm ||r||_B = 1.643757e-11\n",
       " 21 KSP residual norm ||r||_B = 3.500414e-12\n",
       " 22 KSP residual norm ||r||_B = 7.237556e-13\n",
       " 23 KSP residual norm ||r||_B = 1.494668e-13\n",
       " 24 KSP residual norm ||r||_B = 3.423373e-14\n",
       " 25 KSP residual norm ||r||_B = 7.739959e-15\n",
       " 26 KSP residual norm ||r||_B = 1.606443e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.695e-01)\n",
       " Sol. ||E|| = 1.244637e-02, ||B|| = 2.449934e-04\n",
       " Field energy E (1.882e-20 J) + H (3.812e-20 J) = 5.694e-20 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 7\n",
       " Updating solution error estimates\n",
       "\n",
       "It 7/100: t = 3.500000e-02 ns (elapsed time = 3.03e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.225322e-06\n",
       "  1 KSP residual norm ||r||_B = 9.015470e-07\n",
       "  2 KSP residual norm ||r||_B = 7.779833e-07\n",
       "  3 KSP residual norm ||r||_B = 6.805150e-07\n",
       "  4 KSP residual norm ||r||_B = 4.346290e-07\n",
       "  5 KSP residual norm ||r||_B = 2.215935e-07\n",
       "  6 KSP residual norm ||r||_B = 1.049748e-07\n",
       "  7 KSP residual norm ||r||_B = 7.544317e-08\n",
       "  8 KSP residual norm ||r||_B = 1.109195e-07\n",
       "  9 KSP residual norm ||r||_B = 1.981283e-07\n",
       " 10 KSP residual norm ||r||_B = 2.374671e-07\n",
       " 11 KSP residual norm ||r||_B = 2.505373e-07\n",
       " 12 KSP residual norm ||r||_B = 2.809156e-07\n",
       " 13 KSP residual norm ||r||_B = 1.164180e-07\n",
       " 14 KSP residual norm ||r||_B = 3.628750e-08\n",
       " 15 KSP residual norm ||r||_B = 1.339470e-08\n",
       " 16 KSP residual norm ||r||_B = 4.441878e-09\n",
       " 17 KSP residual norm ||r||_B = 1.433494e-09\n",
       " 18 KSP residual norm ||r||_B = 3.819624e-10\n",
       " 19 KSP residual norm ||r||_B = 8.692946e-11\n",
       " 20 KSP residual norm ||r||_B = 1.888483e-11\n",
       " 21 KSP residual norm ||r||_B = 4.036655e-12\n",
       " 22 KSP residual norm ||r||_B = 8.305156e-13\n",
       " 23 KSP residual norm ||r||_B = 1.698638e-13\n",
       " 24 KSP residual norm ||r||_B = 3.913004e-14\n",
       " 25 KSP residual norm ||r||_B = 8.941090e-15\n",
       " 26 KSP residual norm ||r||_B = 1.838401e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.679e-01)\n",
       " Sol. ||E|| = 1.806086e-02, ||B|| = 3.557339e-04\n",
       " Field energy E (3.962e-20 J) + H (8.038e-20 J) = 1.200e-19 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 8/100: t = 4.000000e-02 ns (elapsed time = 3.46e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.345825e-06\n",
       "  1 KSP residual norm ||r||_B = 9.835058e-07\n",
       "  2 KSP residual norm ||r||_B = 8.462749e-07\n",
       "  3 KSP residual norm ||r||_B = 7.386633e-07\n",
       "  4 KSP residual norm ||r||_B = 4.687183e-07\n",
       "  5 KSP residual norm ||r||_B = 2.346025e-07\n",
       "  6 KSP residual norm ||r||_B = 1.008556e-07\n",
       "  7 KSP residual norm ||r||_B = 5.356330e-08\n",
       "  8 KSP residual norm ||r||_B = 5.411533e-08\n",
       "  9 KSP residual norm ||r||_B = 8.014483e-08\n",
       " 10 KSP residual norm ||r||_B = 1.012969e-07\n",
       " 11 KSP residual norm ||r||_B = 1.289453e-07\n",
       " 12 KSP residual norm ||r||_B = 2.150751e-07\n",
       " 13 KSP residual norm ||r||_B = 1.236166e-07\n",
       " 14 KSP residual norm ||r||_B = 4.125369e-08\n",
       " 15 KSP residual norm ||r||_B = 1.541480e-08\n",
       " 16 KSP residual norm ||r||_B = 5.046250e-09\n",
       " 17 KSP residual norm ||r||_B = 1.602471e-09\n",
       " 18 KSP residual norm ||r||_B = 4.219651e-10\n",
       " 19 KSP residual norm ||r||_B = 9.567029e-11\n",
       " 20 KSP residual norm ||r||_B = 2.079565e-11\n",
       " 21 KSP residual norm ||r||_B = 4.448204e-12\n",
       " 22 KSP residual norm ||r||_B = 9.147068e-13\n",
       " 23 KSP residual norm ||r||_B = 1.867076e-13\n",
       " 24 KSP residual norm ||r||_B = 4.306781e-14\n",
       " 25 KSP residual norm ||r||_B = 9.864018e-15\n",
       " 26 KSP residual norm ||r||_B = 2.023912e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.702e-01)\n",
       " Sol. ||E|| = 2.539303e-02, ||B|| = 5.004523e-04\n",
       " Field energy E (7.832e-20 J) + H (1.591e-19 J) = 2.374e-19 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 9\n",
       " Updating solution error estimates\n",
       "\n",
       "It 9/100: t = 4.500000e-02 ns (elapsed time = 3.99e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.460663e-06\n",
       "  1 KSP residual norm ||r||_B = 1.046020e-06\n",
       "  2 KSP residual norm ||r||_B = 8.900011e-07\n",
       "  3 KSP residual norm ||r||_B = 7.839657e-07\n",
       "  4 KSP residual norm ||r||_B = 5.015546e-07\n",
       "  5 KSP residual norm ||r||_B = 2.586342e-07\n",
       "  6 KSP residual norm ||r||_B = 1.173626e-07\n",
       "  7 KSP residual norm ||r||_B = 6.856426e-08\n",
       "  8 KSP residual norm ||r||_B = 6.954769e-08\n",
       "  9 KSP residual norm ||r||_B = 8.677176e-08\n",
       " 10 KSP residual norm ||r||_B = 1.044452e-07\n",
       " 11 KSP residual norm ||r||_B = 1.556587e-07\n",
       " 12 KSP residual norm ||r||_B = 2.689667e-07\n",
       " 13 KSP residual norm ||r||_B = 1.452859e-07\n",
       " 14 KSP residual norm ||r||_B = 5.131049e-08\n",
       " 15 KSP residual norm ||r||_B = 1.899648e-08\n",
       " 16 KSP residual norm ||r||_B = 5.978774e-09\n",
       " 17 KSP residual norm ||r||_B = 1.837654e-09\n",
       " 18 KSP residual norm ||r||_B = 4.672760e-10\n",
       " 19 KSP residual norm ||r||_B = 1.044835e-10\n",
       " 20 KSP residual norm ||r||_B = 2.277633e-11\n",
       " 21 KSP residual norm ||r||_B = 4.885559e-12\n",
       " 22 KSP residual norm ||r||_B = 9.996746e-13\n",
       " 23 KSP residual norm ||r||_B = 2.023291e-13\n",
       " 24 KSP residual norm ||r||_B = 4.691883e-14\n",
       " 25 KSP residual norm ||r||_B = 1.085373e-14\n",
       " 26 KSP residual norm ||r||_B = 2.205347e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.682e-01)\n",
       " Sol. ||E|| = 3.454088e-02, ||B|| = 6.812121e-04\n",
       " Field energy E (1.449e-19 J) + H (2.948e-19 J) = 4.397e-19 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 10/100: t = 5.000000e-02 ns (elapsed time = 4.39e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.592227e-06\n",
       "  1 KSP residual norm ||r||_B = 1.121216e-06\n",
       "  2 KSP residual norm ||r||_B = 9.438648e-07\n",
       "  3 KSP residual norm ||r||_B = 8.355988e-07\n",
       "  4 KSP residual norm ||r||_B = 5.383341e-07\n",
       "  5 KSP residual norm ||r||_B = 2.830957e-07\n",
       "  6 KSP residual norm ||r||_B = 1.316202e-07\n",
       "  7 KSP residual norm ||r||_B = 7.684568e-08\n",
       "  8 KSP residual norm ||r||_B = 7.026711e-08\n",
       "  9 KSP residual norm ||r||_B = 7.432847e-08\n",
       " 10 KSP residual norm ||r||_B = 8.599583e-08\n",
       " 11 KSP residual norm ||r||_B = 1.367089e-07\n",
       " 12 KSP residual norm ||r||_B = 2.638197e-07\n",
       " 13 KSP residual norm ||r||_B = 1.615672e-07\n",
       " 14 KSP residual norm ||r||_B = 6.044726e-08\n",
       " 15 KSP residual norm ||r||_B = 2.207409e-08\n",
       " 16 KSP residual norm ||r||_B = 6.803014e-09\n",
       " 17 KSP residual norm ||r||_B = 2.061376e-09\n",
       " 18 KSP residual norm ||r||_B = 5.149766e-10\n",
       " 19 KSP residual norm ||r||_B = 1.143819e-10\n",
       " 20 KSP residual norm ||r||_B = 2.499873e-11\n",
       " 21 KSP residual norm ||r||_B = 5.369941e-12\n",
       " 22 KSP residual norm ||r||_B = 1.095118e-12\n",
       " 23 KSP residual norm ||r||_B = 2.204245e-13\n",
       " 24 KSP residual norm ||r||_B = 5.129127e-14\n",
       " 25 KSP residual norm ||r||_B = 1.194607e-14\n",
       " 26 KSP residual norm ||r||_B = 2.410584e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.704e-01)\n",
       " Sol. ||E|| = 4.552326e-02, ||B|| = 8.983287e-04\n",
       " Field energy E (2.517e-19 J) + H (5.126e-19 J) = 7.643e-19 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 11\n",
       " Updating solution error estimates\n",
       "\n",
       "It 11/100: t = 5.500000e-02 ns (elapsed time = 4.89e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.652610e-06\n",
       "  1 KSP residual norm ||r||_B = 1.147855e-06\n",
       "  2 KSP residual norm ||r||_B = 9.585142e-07\n",
       "  3 KSP residual norm ||r||_B = 8.497210e-07\n",
       "  4 KSP residual norm ||r||_B = 5.489368e-07\n",
       "  5 KSP residual norm ||r||_B = 2.898176e-07\n",
       "  6 KSP residual norm ||r||_B = 1.323088e-07\n",
       "  7 KSP residual norm ||r||_B = 6.803152e-08\n",
       "  8 KSP residual norm ||r||_B = 4.466175e-08\n",
       "  9 KSP residual norm ||r||_B = 2.756237e-08\n",
       " 10 KSP residual norm ||r||_B = 1.566645e-08\n",
       " 11 KSP residual norm ||r||_B = 1.314107e-08\n",
       " 12 KSP residual norm ||r||_B = 2.791242e-08\n",
       " 13 KSP residual norm ||r||_B = 6.134301e-08\n",
       " 14 KSP residual norm ||r||_B = 5.198819e-08\n",
       " 15 KSP residual norm ||r||_B = 2.307215e-08\n",
       " 16 KSP residual norm ||r||_B = 7.203849e-09\n",
       " 17 KSP residual norm ||r||_B = 2.171236e-09\n",
       " 18 KSP residual norm ||r||_B = 5.379722e-10\n",
       " 19 KSP residual norm ||r||_B = 1.191438e-10\n",
       " 20 KSP residual norm ||r||_B = 2.608649e-11\n",
       " 21 KSP residual norm ||r||_B = 5.607334e-12\n",
       " 22 KSP residual norm ||r||_B = 1.141792e-12\n",
       " 23 KSP residual norm ||r||_B = 2.290563e-13\n",
       " 24 KSP residual norm ||r||_B = 5.339453e-14\n",
       " 25 KSP residual norm ||r||_B = 1.248811e-14\n",
       " 26 KSP residual norm ||r||_B = 2.510269e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.692e-01)\n",
       " Sol. ||E|| = 5.790174e-02, ||B|| = 1.143513e-03\n",
       " Field energy E (4.072e-19 J) + H (8.306e-19 J) = 1.238e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 12/100: t = 6.000000e-02 ns (elapsed time = 5.29e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.859021e-06\n",
       "  1 KSP residual norm ||r||_B = 1.250034e-06\n",
       "  2 KSP residual norm ||r||_B = 1.013383e-06\n",
       "  3 KSP residual norm ||r||_B = 9.058161e-07\n",
       "  4 KSP residual norm ||r||_B = 6.029655e-07\n",
       "  5 KSP residual norm ||r||_B = 3.459459e-07\n",
       "  6 KSP residual norm ||r||_B = 1.883639e-07\n",
       "  7 KSP residual norm ||r||_B = 1.332031e-07\n",
       "  8 KSP residual norm ||r||_B = 1.253476e-07\n",
       "  9 KSP residual norm ||r||_B = 1.294334e-07\n",
       " 10 KSP residual norm ||r||_B = 1.729632e-07\n",
       " 11 KSP residual norm ||r||_B = 3.014821e-07\n",
       " 12 KSP residual norm ||r||_B = 4.584397e-07\n",
       " 13 KSP residual norm ||r||_B = 2.221829e-07\n",
       " 14 KSP residual norm ||r||_B = 8.369688e-08\n",
       " 15 KSP residual norm ||r||_B = 2.869481e-08\n",
       " 16 KSP residual norm ||r||_B = 8.577281e-09\n",
       " 17 KSP residual norm ||r||_B = 2.549109e-09\n",
       " 18 KSP residual norm ||r||_B = 6.152503e-10\n",
       " 19 KSP residual norm ||r||_B = 1.350584e-10\n",
       " 20 KSP residual norm ||r||_B = 2.970827e-11\n",
       " 21 KSP residual norm ||r||_B = 6.385539e-12\n",
       " 22 KSP residual norm ||r||_B = 1.291905e-12\n",
       " 23 KSP residual norm ||r||_B = 2.574389e-13\n",
       " 24 KSP residual norm ||r||_B = 6.033382e-14\n",
       " 25 KSP residual norm ||r||_B = 1.424556e-14\n",
       " 26 KSP residual norm ||r||_B = 2.831240e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.694e-01)\n",
       " Sol. ||E|| = 7.079685e-02, ||B|| = 1.399286e-03\n",
       " Field energy E (6.088e-19 J) + H (1.244e-18 J) = 1.853e-18 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 13\n",
       " Updating solution error estimates\n",
       "\n",
       "It 13/100: t = 6.500000e-02 ns (elapsed time = 5.80e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.801971e-06\n",
       "  1 KSP residual norm ||r||_B = 1.218182e-06\n",
       "  2 KSP residual norm ||r||_B = 1.001496e-06\n",
       "  3 KSP residual norm ||r||_B = 8.948829e-07\n",
       "  4 KSP residual norm ||r||_B = 5.898723e-07\n",
       "  5 KSP residual norm ||r||_B = 3.250863e-07\n",
       "  6 KSP residual norm ||r||_B = 1.648329e-07\n",
       "  7 KSP residual norm ||r||_B = 1.055011e-07\n",
       "  8 KSP residual norm ||r||_B = 9.385013e-08\n",
       "  9 KSP residual norm ||r||_B = 9.170160e-08\n",
       " 10 KSP residual norm ||r||_B = 1.113828e-07\n",
       " 11 KSP residual norm ||r||_B = 1.887624e-07\n",
       " 12 KSP residual norm ||r||_B = 3.460643e-07\n",
       " 13 KSP residual norm ||r||_B = 2.010917e-07\n",
       " 14 KSP residual norm ||r||_B = 7.765734e-08\n",
       " 15 KSP residual norm ||r||_B = 2.730875e-08\n",
       " 16 KSP residual norm ||r||_B = 8.145596e-09\n",
       " 17 KSP residual norm ||r||_B = 2.426623e-09\n",
       " 18 KSP residual norm ||r||_B = 5.940677e-10\n",
       " 19 KSP residual norm ||r||_B = 1.310091e-10\n",
       " 20 KSP residual norm ||r||_B = 2.877317e-11\n",
       " 21 KSP residual norm ||r||_B = 6.190357e-12\n",
       " 22 KSP residual norm ||r||_B = 1.257427e-12\n",
       " 23 KSP residual norm ||r||_B = 2.508085e-13\n",
       " 24 KSP residual norm ||r||_B = 5.858747e-14\n",
       " 25 KSP residual norm ||r||_B = 1.380105e-14\n",
       " 26 KSP residual norm ||r||_B = 2.758320e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.721e-01)\n",
       " Sol. ||E|| = 8.242342e-02, ||B|| = 1.630951e-03\n",
       " Field energy E (8.252e-19 J) + H (1.690e-18 J) = 2.515e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 14/100: t = 7.000000e-02 ns (elapsed time = 6.20e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 2.190527e-06\n",
       "  1 KSP residual norm ||r||_B = 1.406188e-06\n",
       "  2 KSP residual norm ||r||_B = 1.084379e-06\n",
       "  3 KSP residual norm ||r||_B = 9.668981e-07\n",
       "  4 KSP residual norm ||r||_B = 6.771416e-07\n",
       "  5 KSP residual norm ||r||_B = 4.438396e-07\n",
       "  6 KSP residual norm ||r||_B = 3.006162e-07\n",
       "  7 KSP residual norm ||r||_B = 2.577938e-07\n",
       "  8 KSP residual norm ||r||_B = 2.603279e-07\n",
       "  9 KSP residual norm ||r||_B = 3.066900e-07\n",
       " 10 KSP residual norm ||r||_B = 4.766537e-07\n",
       " 11 KSP residual norm ||r||_B = 7.634594e-07\n",
       " 12 KSP residual norm ||r||_B = 7.566039e-07\n",
       " 13 KSP residual norm ||r||_B = 2.982134e-07\n",
       " 14 KSP residual norm ||r||_B = 1.093423e-07\n",
       " 15 KSP residual norm ||r||_B = 3.569093e-08\n",
       " 16 KSP residual norm ||r||_B = 1.058700e-08\n",
       " 17 KSP residual norm ||r||_B = 3.121761e-09\n",
       " 18 KSP residual norm ||r||_B = 7.400869e-10\n",
       " 19 KSP residual norm ||r||_B = 1.618805e-10\n",
       " 20 KSP residual norm ||r||_B = 3.564570e-11\n",
       " 21 KSP residual norm ||r||_B = 7.613678e-12\n",
       " 22 KSP residual norm ||r||_B = 1.538972e-12\n",
       " 23 KSP residual norm ||r||_B = 3.080257e-13\n",
       " 24 KSP residual norm ||r||_B = 7.216300e-14\n",
       " 25 KSP residual norm ||r||_B = 1.700313e-14\n",
       " 26 KSP residual norm ||r||_B = 3.390667e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.662e-01)\n",
       " Sol. ||E|| = 8.997379e-02, ||B|| = 1.782948e-03\n",
       " Field energy E (9.833e-19 J) + H (2.019e-18 J) = 3.003e-18 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 15\n",
       " Updating solution error estimates\n",
       "\n",
       "It 15/100: t = 7.500000e-02 ns (elapsed time = 6.72e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.906501e-06\n",
       "  1 KSP residual norm ||r||_B = 1.270843e-06\n",
       "  2 KSP residual norm ||r||_B = 1.048413e-06\n",
       "  3 KSP residual norm ||r||_B = 9.602273e-07\n",
       "  4 KSP residual norm ||r||_B = 6.639714e-07\n",
       "  5 KSP residual norm ||r||_B = 4.047788e-07\n",
       "  6 KSP residual norm ||r||_B = 2.694953e-07\n",
       "  7 KSP residual norm ||r||_B = 2.749483e-07\n",
       "  8 KSP residual norm ||r||_B = 3.839502e-07\n",
       "  9 KSP residual norm ||r||_B = 5.019312e-07\n",
       " 10 KSP residual norm ||r||_B = 6.659890e-07\n",
       " 11 KSP residual norm ||r||_B = 8.817623e-07\n",
       " 12 KSP residual norm ||r||_B = 6.835906e-07\n",
       " 13 KSP residual norm ||r||_B = 2.373641e-07\n",
       " 14 KSP residual norm ||r||_B = 8.557859e-08\n",
       " 15 KSP residual norm ||r||_B = 2.958534e-08\n",
       " 16 KSP residual norm ||r||_B = 8.715434e-09\n",
       " 17 KSP residual norm ||r||_B = 2.588998e-09\n",
       " 18 KSP residual norm ||r||_B = 6.341331e-10\n",
       " 19 KSP residual norm ||r||_B = 1.398667e-10\n",
       " 20 KSP residual norm ||r||_B = 3.075576e-11\n",
       " 21 KSP residual norm ||r||_B = 6.623425e-12\n",
       " 22 KSP residual norm ||r||_B = 1.345423e-12\n",
       " 23 KSP residual norm ||r||_B = 2.673177e-13\n",
       " 24 KSP residual norm ||r||_B = 6.235442e-14\n",
       " 25 KSP residual norm ||r||_B = 1.474336e-14\n",
       " 26 KSP residual norm ||r||_B = 2.946411e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.743e-01)\n",
       " Sol. ||E|| = 8.908027e-02, ||B|| = 1.769677e-03\n",
       " Field energy E (9.639e-19 J) + H (1.989e-18 J) = 2.953e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 16/100: t = 8.000000e-02 ns (elapsed time = 7.13e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 2.622519e-06\n",
       "  1 KSP residual norm ||r||_B = 1.626997e-06\n",
       "  2 KSP residual norm ||r||_B = 1.197443e-06\n",
       "  3 KSP residual norm ||r||_B = 1.056020e-06\n",
       "  4 KSP residual norm ||r||_B = 7.909570e-07\n",
       "  5 KSP residual norm ||r||_B = 6.180704e-07\n",
       "  6 KSP residual norm ||r||_B = 5.343503e-07\n",
       "  7 KSP residual norm ||r||_B = 5.295331e-07\n",
       "  8 KSP residual norm ||r||_B = 5.571851e-07\n",
       "  9 KSP residual norm ||r||_B = 7.237312e-07\n",
       " 10 KSP residual norm ||r||_B = 1.157614e-06\n",
       " 11 KSP residual norm ||r||_B = 1.480638e-06\n",
       " 12 KSP residual norm ||r||_B = 1.056239e-06\n",
       " 13 KSP residual norm ||r||_B = 3.837292e-07\n",
       " 14 KSP residual norm ||r||_B = 1.365966e-07\n",
       " 15 KSP residual norm ||r||_B = 4.357429e-08\n",
       " 16 KSP residual norm ||r||_B = 1.295160e-08\n",
       " 17 KSP residual norm ||r||_B = 3.811460e-09\n",
       " 18 KSP residual norm ||r||_B = 9.041795e-10\n",
       " 19 KSP residual norm ||r||_B = 1.985408e-10\n",
       " 20 KSP residual norm ||r||_B = 4.335712e-11\n",
       " 21 KSP residual norm ||r||_B = 9.136444e-12\n",
       " 22 KSP residual norm ||r||_B = 1.864296e-12\n",
       " 23 KSP residual norm ||r||_B = 3.810139e-13\n",
       " 24 KSP residual norm ||r||_B = 8.823890e-14\n",
       " 25 KSP residual norm ||r||_B = 2.037342e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.760e-01)\n",
       " Sol. ||E|| = 7.361529e-02, ||B|| = 1.469963e-03\n",
       " Field energy E (6.583e-19 J) + H (1.373e-18 J) = 2.031e-18 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 17\n",
       " Updating solution error estimates\n",
       "\n",
       "It 17/100: t = 8.500000e-02 ns (elapsed time = 7.64e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.981081e-06\n",
       "  1 KSP residual norm ||r||_B = 1.334284e-06\n",
       "  2 KSP residual norm ||r||_B = 1.147806e-06\n",
       "  3 KSP residual norm ||r||_B = 1.117827e-06\n",
       "  4 KSP residual norm ||r||_B = 8.470136e-07\n",
       "  5 KSP residual norm ||r||_B = 6.053222e-07\n",
       "  6 KSP residual norm ||r||_B = 5.418702e-07\n",
       "  7 KSP residual norm ||r||_B = 7.511668e-07\n",
       "  8 KSP residual norm ||r||_B = 1.205376e-06\n",
       "  9 KSP residual norm ||r||_B = 1.444852e-06\n",
       " 10 KSP residual norm ||r||_B = 1.454932e-06\n",
       " 11 KSP residual norm ||r||_B = 1.354442e-06\n",
       " 12 KSP residual norm ||r||_B = 7.641050e-07\n",
       " 13 KSP residual norm ||r||_B = 2.452406e-07\n",
       " 14 KSP residual norm ||r||_B = 8.740834e-08\n",
       " 15 KSP residual norm ||r||_B = 3.065353e-08\n",
       " 16 KSP residual norm ||r||_B = 8.966506e-09\n",
       " 17 KSP residual norm ||r||_B = 2.663556e-09\n",
       " 18 KSP residual norm ||r||_B = 6.604777e-10\n",
       " 19 KSP residual norm ||r||_B = 1.464333e-10\n",
       " 20 KSP residual norm ||r||_B = 3.218082e-11\n",
       " 21 KSP residual norm ||r||_B = 6.941402e-12\n",
       " 22 KSP residual norm ||r||_B = 1.413024e-12\n",
       " 23 KSP residual norm ||r||_B = 2.799537e-13\n",
       " 24 KSP residual norm ||r||_B = 6.499947e-14\n",
       " 25 KSP residual norm ||r||_B = 1.538546e-14\n",
       " 26 KSP residual norm ||r||_B = 3.089994e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.629e-01)\n",
       " Sol. ||E|| = 3.518896e-02, ||B|| = 7.185047e-04\n",
       " Field energy E (1.504e-19 J) + H (3.280e-19 J) = 4.784e-19 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 18/100: t = 9.000000e-02 ns (elapsed time = 8.05e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 3.154480e-06\n",
       "  1 KSP residual norm ||r||_B = 1.926624e-06\n",
       "  2 KSP residual norm ||r||_B = 1.380010e-06\n",
       "  3 KSP residual norm ||r||_B = 1.209301e-06\n",
       "  4 KSP residual norm ||r||_B = 9.768643e-07\n",
       "  5 KSP residual norm ||r||_B = 9.153944e-07\n",
       "  6 KSP residual norm ||r||_B = 9.862816e-07\n",
       "  7 KSP residual norm ||r||_B = 1.058662e-06\n",
       "  8 KSP residual norm ||r||_B = 1.082286e-06\n",
       "  9 KSP residual norm ||r||_B = 1.413550e-06\n",
       " 10 KSP residual norm ||r||_B = 2.127520e-06\n",
       " 11 KSP residual norm ||r||_B = 2.166503e-06\n",
       " 12 KSP residual norm ||r||_B = 1.328428e-06\n",
       " 13 KSP residual norm ||r||_B = 4.752921e-07\n",
       " 14 KSP residual norm ||r||_B = 1.645276e-07\n",
       " 15 KSP residual norm ||r||_B = 5.218824e-08\n",
       " 16 KSP residual norm ||r||_B = 1.558213e-08\n",
       " 17 KSP residual norm ||r||_B = 4.594999e-09\n",
       " 18 KSP residual norm ||r||_B = 1.105423e-09\n",
       " 19 KSP residual norm ||r||_B = 2.446267e-10\n",
       " 20 KSP residual norm ||r||_B = 5.267771e-11\n",
       " 21 KSP residual norm ||r||_B = 1.091915e-11\n",
       " 22 KSP residual norm ||r||_B = 2.258121e-12\n",
       " 23 KSP residual norm ||r||_B = 4.730446e-13\n",
       " 24 KSP residual norm ||r||_B = 1.077075e-13\n",
       " 25 KSP residual norm ||r||_B = 2.427904e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.692e-01)\n",
       " Sol. ||E|| = 3.712086e-02, ||B|| = 6.990641e-04\n",
       " Field energy E (1.673e-19 J) + H (3.103e-19 J) = 4.777e-19 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 19\n",
       " Updating solution error estimates\n",
       "\n",
       "It 19/100: t = 9.500000e-02 ns (elapsed time = 8.55e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 2.070057e-06\n",
       "  1 KSP residual norm ||r||_B = 1.442683e-06\n",
       "  2 KSP residual norm ||r||_B = 1.337346e-06\n",
       "  3 KSP residual norm ||r||_B = 1.419424e-06\n",
       "  4 KSP residual norm ||r||_B = 1.192307e-06\n",
       "  5 KSP residual norm ||r||_B = 9.685902e-07\n",
       "  6 KSP residual norm ||r||_B = 1.027703e-06\n",
       "  7 KSP residual norm ||r||_B = 1.609940e-06\n",
       "  8 KSP residual norm ||r||_B = 2.549321e-06\n",
       "  9 KSP residual norm ||r||_B = 2.429906e-06\n",
       " 10 KSP residual norm ||r||_B = 1.790769e-06\n",
       " 11 KSP residual norm ||r||_B = 1.400252e-06\n",
       " 12 KSP residual norm ||r||_B = 7.703593e-07\n",
       " 13 KSP residual norm ||r||_B = 2.448409e-07\n",
       " 14 KSP residual norm ||r||_B = 8.579051e-08\n",
       " 15 KSP residual norm ||r||_B = 3.107152e-08\n",
       " 16 KSP residual norm ||r||_B = 9.089758e-09\n",
       " 17 KSP residual norm ||r||_B = 2.698986e-09\n",
       " 18 KSP residual norm ||r||_B = 6.833671e-10\n",
       " 19 KSP residual norm ||r||_B = 1.531259e-10\n",
       " 20 KSP residual norm ||r||_B = 3.360062e-11\n",
       " 21 KSP residual norm ||r||_B = 7.255663e-12\n",
       " 22 KSP residual norm ||r||_B = 1.483266e-12\n",
       " 23 KSP residual norm ||r||_B = 2.938232e-13\n",
       " 24 KSP residual norm ||r||_B = 6.779420e-14\n",
       " 25 KSP residual norm ||r||_B = 1.601703e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.648e-01)\n",
       " Sol. ||E|| = 1.566086e-01, ||B|| = 3.047965e-03\n",
       " Field energy E (2.979e-18 J) + H (5.901e-18 J) = 8.879e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 20/100: t = 1.000000e-01 ns (elapsed time = 8.95e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 3.712494e-06\n",
       "  1 KSP residual norm ||r||_B = 2.258531e-06\n",
       "  2 KSP residual norm ||r||_B = 1.600695e-06\n",
       "  3 KSP residual norm ||r||_B = 1.399605e-06\n",
       "  4 KSP residual norm ||r||_B = 1.201917e-06\n",
       "  5 KSP residual norm ||r||_B = 1.291836e-06\n",
       "  6 KSP residual norm ||r||_B = 1.645008e-06\n",
       "  7 KSP residual norm ||r||_B = 1.850942e-06\n",
       "  8 KSP residual norm ||r||_B = 1.745809e-06\n",
       "  9 KSP residual norm ||r||_B = 2.124784e-06\n",
       " 10 KSP residual norm ||r||_B = 2.961762e-06\n",
       " 11 KSP residual norm ||r||_B = 2.614473e-06\n",
       " 12 KSP residual norm ||r||_B = 1.545131e-06\n",
       " 13 KSP residual norm ||r||_B = 5.615183e-07\n",
       " 14 KSP residual norm ||r||_B = 1.900810e-07\n",
       " 15 KSP residual norm ||r||_B = 6.035744e-08\n",
       " 16 KSP residual norm ||r||_B = 1.810050e-08\n",
       " 17 KSP residual norm ||r||_B = 5.360760e-09\n",
       " 18 KSP residual norm ||r||_B = 1.313137e-09\n",
       " 19 KSP residual norm ||r||_B = 2.929608e-10\n",
       " 20 KSP residual norm ||r||_B = 6.226923e-11\n",
       " 21 KSP residual norm ||r||_B = 1.272025e-11\n",
       " 22 KSP residual norm ||r||_B = 2.657596e-12\n",
       " 23 KSP residual norm ||r||_B = 5.673772e-13\n",
       " 24 KSP residual norm ||r||_B = 1.273728e-13\n",
       " 25 KSP residual norm ||r||_B = 2.820274e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.630e-01)\n",
       " Sol. ||E|| = 3.393702e-01, ||B|| = 6.645061e-03\n",
       " Field energy E (1.399e-17 J) + H (2.805e-17 J) = 4.204e-17 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 21\n",
       " Updating solution error estimates\n",
       "\n",
       "It 21/100: t = 1.050000e-01 ns (elapsed time = 9.48e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 2.225153e-06\n",
       "  1 KSP residual norm ||r||_B = 1.581807e-06\n",
       "  2 KSP residual norm ||r||_B = 1.544660e-06\n",
       "  3 KSP residual norm ||r||_B = 1.749931e-06\n",
       "  4 KSP residual norm ||r||_B = 1.578894e-06\n",
       "  5 KSP residual norm ||r||_B = 1.357967e-06\n",
       "  6 KSP residual norm ||r||_B = 1.514440e-06\n",
       "  7 KSP residual norm ||r||_B = 2.412357e-06\n",
       "  8 KSP residual norm ||r||_B = 3.621270e-06\n",
       "  9 KSP residual norm ||r||_B = 2.956921e-06\n",
       " 10 KSP residual norm ||r||_B = 1.869358e-06\n",
       " 11 KSP residual norm ||r||_B = 1.379005e-06\n",
       " 12 KSP residual norm ||r||_B = 7.925884e-07\n",
       " 13 KSP residual norm ||r||_B = 2.547220e-07\n",
       " 14 KSP residual norm ||r||_B = 8.786289e-08\n",
       " 15 KSP residual norm ||r||_B = 3.253796e-08\n",
       " 16 KSP residual norm ||r||_B = 9.559253e-09\n",
       " 17 KSP residual norm ||r||_B = 2.836637e-09\n",
       " 18 KSP residual norm ||r||_B = 7.283264e-10\n",
       " 19 KSP residual norm ||r||_B = 1.644742e-10\n",
       " 20 KSP residual norm ||r||_B = 3.607909e-11\n",
       " 21 KSP residual norm ||r||_B = 7.797088e-12\n",
       " 22 KSP residual norm ||r||_B = 1.599014e-12\n",
       " 23 KSP residual norm ||r||_B = 3.165833e-13\n",
       " 24 KSP residual norm ||r||_B = 7.271754e-14\n",
       " 25 KSP residual norm ||r||_B = 1.717363e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.555e-01)\n",
       " Sol. ||E|| = 6.035673e-01, ||B|| = 1.184982e-02\n",
       " Field energy E (4.425e-17 J) + H (8.919e-17 J) = 1.334e-16 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 22/100: t = 1.100000e-01 ns (elapsed time = 9.88e+02 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 4.128953e-06\n",
       "  1 KSP residual norm ||r||_B = 2.494388e-06\n",
       "  2 KSP residual norm ||r||_B = 1.743180e-06\n",
       "  3 KSP residual norm ||r||_B = 1.497168e-06\n",
       "  4 KSP residual norm ||r||_B = 1.309653e-06\n",
       "  5 KSP residual norm ||r||_B = 1.501279e-06\n",
       "  6 KSP residual norm ||r||_B = 2.129392e-06\n",
       "  7 KSP residual norm ||r||_B = 2.525184e-06\n",
       "  8 KSP residual norm ||r||_B = 2.198148e-06\n",
       "  9 KSP residual norm ||r||_B = 2.413241e-06\n",
       " 10 KSP residual norm ||r||_B = 3.224167e-06\n",
       " 11 KSP residual norm ||r||_B = 2.736882e-06\n",
       " 12 KSP residual norm ||r||_B = 1.656966e-06\n",
       " 13 KSP residual norm ||r||_B = 6.207919e-07\n",
       " 14 KSP residual norm ||r||_B = 2.074252e-07\n",
       " 15 KSP residual norm ||r||_B = 6.600119e-08\n",
       " 16 KSP residual norm ||r||_B = 1.984908e-08\n",
       " 17 KSP residual norm ||r||_B = 5.904517e-09\n",
       " 18 KSP residual norm ||r||_B = 1.467880e-09\n",
       " 19 KSP residual norm ||r||_B = 3.295518e-10\n",
       " 20 KSP residual norm ||r||_B = 6.947955e-11\n",
       " 21 KSP residual norm ||r||_B = 1.405252e-11\n",
       " 22 KSP residual norm ||r||_B = 2.951557e-12\n",
       " 23 KSP residual norm ||r||_B = 6.371535e-13\n",
       " 24 KSP residual norm ||r||_B = 1.418795e-13\n",
       " 25 KSP residual norm ||r||_B = 3.108884e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.578e-01)\n",
       " Sol. ||E|| = 9.687307e-01, ||B|| = 1.904971e-02\n",
       " Field energy E (1.140e-16 J) + H (2.305e-16 J) = 3.445e-16 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 23\n",
       " Updating solution error estimates\n",
       "\n",
       "It 23/100: t = 1.150000e-01 ns (elapsed time = 1.04e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 2.490085e-06\n",
       "  1 KSP residual norm ||r||_B = 1.674278e-06\n",
       "  2 KSP residual norm ||r||_B = 1.557176e-06\n",
       "  3 KSP residual norm ||r||_B = 1.767568e-06\n",
       "  4 KSP residual norm ||r||_B = 1.644077e-06\n",
       "  5 KSP residual norm ||r||_B = 1.431192e-06\n",
       "  6 KSP residual norm ||r||_B = 1.538288e-06\n",
       "  7 KSP residual norm ||r||_B = 2.305316e-06\n",
       "  8 KSP residual norm ||r||_B = 3.382005e-06\n",
       "  9 KSP residual norm ||r||_B = 3.110966e-06\n",
       " 10 KSP residual norm ||r||_B = 2.347928e-06\n",
       " 11 KSP residual norm ||r||_B = 1.815145e-06\n",
       " 12 KSP residual norm ||r||_B = 9.629819e-07\n",
       " 13 KSP residual norm ||r||_B = 3.050576e-07\n",
       " 14 KSP residual norm ||r||_B = 1.072217e-07\n",
       " 15 KSP residual norm ||r||_B = 3.854724e-08\n",
       " 16 KSP residual norm ||r||_B = 1.119533e-08\n",
       " 17 KSP residual norm ||r||_B = 3.327112e-09\n",
       " 18 KSP residual norm ||r||_B = 8.396957e-10\n",
       " 19 KSP residual norm ||r||_B = 1.871584e-10\n",
       " 20 KSP residual norm ||r||_B = 4.111869e-11\n",
       " 21 KSP residual norm ||r||_B = 8.906409e-12\n",
       " 22 KSP residual norm ||r||_B = 1.821005e-12\n",
       " 23 KSP residual norm ||r||_B = 3.575024e-13\n",
       " 24 KSP residual norm ||r||_B = 8.215850e-14\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.629e-01)\n",
       " Sol. ||E|| = 1.454653e+00, ||B|| = 2.863724e-02\n",
       " Field energy E (2.570e-16 J) + H (5.209e-16 J) = 7.779e-16 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 24/100: t = 1.200000e-01 ns (elapsed time = 1.08e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 4.172970e-06\n",
       "  1 KSP residual norm ||r||_B = 2.454401e-06\n",
       "  2 KSP residual norm ||r||_B = 1.643265e-06\n",
       "  3 KSP residual norm ||r||_B = 1.321881e-06\n",
       "  4 KSP residual norm ||r||_B = 1.082560e-06\n",
       "  5 KSP residual norm ||r||_B = 1.185668e-06\n",
       "  6 KSP residual norm ||r||_B = 1.730565e-06\n",
       "  7 KSP residual norm ||r||_B = 2.212614e-06\n",
       "  8 KSP residual norm ||r||_B = 1.905747e-06\n",
       "  9 KSP residual norm ||r||_B = 1.947492e-06\n",
       " 10 KSP residual norm ||r||_B = 2.657108e-06\n",
       " 11 KSP residual norm ||r||_B = 2.447148e-06\n",
       " 12 KSP residual norm ||r||_B = 1.608903e-06\n",
       " 13 KSP residual norm ||r||_B = 6.257789e-07\n",
       " 14 KSP residual norm ||r||_B = 2.090702e-07\n",
       " 15 KSP residual norm ||r||_B = 6.665871e-08\n",
       " 16 KSP residual norm ||r||_B = 2.003493e-08\n",
       " 17 KSP residual norm ||r||_B = 5.972057e-09\n",
       " 18 KSP residual norm ||r||_B = 1.493674e-09\n",
       " 19 KSP residual norm ||r||_B = 3.360734e-10\n",
       " 20 KSP residual norm ||r||_B = 7.075718e-11\n",
       " 21 KSP residual norm ||r||_B = 1.426612e-11\n",
       " 22 KSP residual norm ||r||_B = 3.000226e-12\n",
       " 23 KSP residual norm ||r||_B = 6.489805e-13\n",
       " 24 KSP residual norm ||r||_B = 1.442819e-13\n",
       " 25 KSP residual norm ||r||_B = 3.153543e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.533e-01)\n",
       " Sol. ||E|| = 2.079668e+00, ||B|| = 4.097738e-02\n",
       " Field energy E (5.253e-16 J) + H (1.067e-15 J) = 1.592e-15 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 25\n",
       " Updating solution error estimates\n",
       "\n",
       "It 25/100: t = 1.250000e-01 ns (elapsed time = 1.13e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 3.007788e-06\n",
       "  1 KSP residual norm ||r||_B = 1.772341e-06\n",
       "  2 KSP residual norm ||r||_B = 1.339347e-06\n",
       "  3 KSP residual norm ||r||_B = 1.296935e-06\n",
       "  4 KSP residual norm ||r||_B = 1.116289e-06\n",
       "  5 KSP residual norm ||r||_B = 9.290565e-07\n",
       "  6 KSP residual norm ||r||_B = 8.692294e-07\n",
       "  7 KSP residual norm ||r||_B = 1.032091e-06\n",
       "  8 KSP residual norm ||r||_B = 1.324325e-06\n",
       "  9 KSP residual norm ||r||_B = 1.632026e-06\n",
       " 10 KSP residual norm ||r||_B = 2.093530e-06\n",
       " 11 KSP residual norm ||r||_B = 2.168540e-06\n",
       " 12 KSP residual norm ||r||_B = 1.267000e-06\n",
       " 13 KSP residual norm ||r||_B = 4.240408e-07\n",
       " 14 KSP residual norm ||r||_B = 1.523740e-07\n",
       " 15 KSP residual norm ||r||_B = 5.082810e-08\n",
       " 16 KSP residual norm ||r||_B = 1.473664e-08\n",
       " 17 KSP residual norm ||r||_B = 4.378134e-09\n",
       " 18 KSP residual norm ||r||_B = 1.061189e-09\n",
       " 19 KSP residual norm ||r||_B = 2.319331e-10\n",
       " 20 KSP residual norm ||r||_B = 5.108414e-11\n",
       " 21 KSP residual norm ||r||_B = 1.100216e-11\n",
       " 22 KSP residual norm ||r||_B = 2.239031e-12\n",
       " 23 KSP residual norm ||r||_B = 4.401982e-13\n",
       " 24 KSP residual norm ||r||_B = 1.016841e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.628e-01)\n",
       " Sol. ||E|| = 2.858673e+00, ||B|| = 5.636724e-02\n",
       " Field energy E (9.926e-16 J) + H (2.018e-15 J) = 3.011e-15 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 26/100: t = 1.300000e-01 ns (elapsed time = 1.16e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 3.668257e-06\n",
       "  1 KSP residual norm ||r||_B = 2.032042e-06\n",
       "  2 KSP residual norm ||r||_B = 1.245359e-06\n",
       "  3 KSP residual norm ||r||_B = 8.647465e-07\n",
       "  4 KSP residual norm ||r||_B = 5.441322e-07\n",
       "  5 KSP residual norm ||r||_B = 3.955209e-07\n",
       "  6 KSP residual norm ||r||_B = 4.048237e-07\n",
       "  7 KSP residual norm ||r||_B = 4.584769e-07\n",
       "  8 KSP residual norm ||r||_B = 3.863861e-07\n",
       "  9 KSP residual norm ||r||_B = 3.656353e-07\n",
       " 10 KSP residual norm ||r||_B = 5.661185e-07\n",
       " 11 KSP residual norm ||r||_B = 8.424669e-07\n",
       " 12 KSP residual norm ||r||_B = 1.030396e-06\n",
       " 13 KSP residual norm ||r||_B = 5.321741e-07\n",
       " 14 KSP residual norm ||r||_B = 1.881796e-07\n",
       " 15 KSP residual norm ||r||_B = 6.046211e-08\n",
       " 16 KSP residual norm ||r||_B = 1.802259e-08\n",
       " 17 KSP residual norm ||r||_B = 5.359830e-09\n",
       " 18 KSP residual norm ||r||_B = 1.328593e-09\n",
       " 19 KSP residual norm ||r||_B = 2.970838e-10\n",
       " 20 KSP residual norm ||r||_B = 6.313347e-11\n",
       " 21 KSP residual norm ||r||_B = 1.284608e-11\n",
       " 22 KSP residual norm ||r||_B = 2.692242e-12\n",
       " 23 KSP residual norm ||r||_B = 5.746631e-13\n",
       " 24 KSP residual norm ||r||_B = 1.287293e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.629e-01)\n",
       " Sol. ||E|| = 3.800693e+00, ||B|| = 7.498892e-02\n",
       " Field energy E (1.755e-15 J) + H (3.572e-15 J) = 5.327e-15 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 27\n",
       " Updating solution error estimates\n",
       "\n",
       "It 27/100: t = 1.350000e-01 ns (elapsed time = 1.21e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 4.097400e-06\n",
       "  1 KSP residual norm ||r||_B = 2.276660e-06\n",
       "  2 KSP residual norm ||r||_B = 1.449082e-06\n",
       "  3 KSP residual norm ||r||_B = 1.107825e-06\n",
       "  4 KSP residual norm ||r||_B = 7.654736e-07\n",
       "  5 KSP residual norm ||r||_B = 5.556441e-07\n",
       "  6 KSP residual norm ||r||_B = 4.466334e-07\n",
       "  7 KSP residual norm ||r||_B = 3.617419e-07\n",
       "  8 KSP residual norm ||r||_B = 2.567679e-07\n",
       "  9 KSP residual norm ||r||_B = 2.154207e-07\n",
       " 10 KSP residual norm ||r||_B = 3.009564e-07\n",
       " 11 KSP residual norm ||r||_B = 5.092190e-07\n",
       " 12 KSP residual norm ||r||_B = 8.720903e-07\n",
       " 13 KSP residual norm ||r||_B = 5.605615e-07\n",
       " 14 KSP residual norm ||r||_B = 2.153157e-07\n",
       " 15 KSP residual norm ||r||_B = 6.986940e-08\n",
       " 16 KSP residual norm ||r||_B = 2.068655e-08\n",
       " 17 KSP residual norm ||r||_B = 6.118765e-09\n",
       " 18 KSP residual norm ||r||_B = 1.474614e-09\n",
       " 19 KSP residual norm ||r||_B = 3.243995e-10\n",
       " 20 KSP residual norm ||r||_B = 7.030107e-11\n",
       " 21 KSP residual norm ||r||_B = 1.470245e-11\n",
       " 22 KSP residual norm ||r||_B = 3.037375e-12\n",
       " 23 KSP residual norm ||r||_B = 6.255459e-13\n",
       " 24 KSP residual norm ||r||_B = 1.427965e-13\n",
       " 25 KSP residual norm ||r||_B = 3.266962e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.559e-01)\n",
       " Sol. ||E|| = 4.906400e+00, ||B|| = 9.685944e-02\n",
       " Field energy E (2.924e-15 J) + H (5.959e-15 J) = 8.883e-15 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 28/100: t = 1.400000e-01 ns (elapsed time = 1.25e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 2.779108e-06\n",
       "  1 KSP residual norm ||r||_B = 1.561358e-06\n",
       "  2 KSP residual norm ||r||_B = 1.158915e-06\n",
       "  3 KSP residual norm ||r||_B = 1.186442e-06\n",
       "  4 KSP residual norm ||r||_B = 1.263240e-06\n",
       "  5 KSP residual norm ||r||_B = 1.450463e-06\n",
       "  6 KSP residual norm ||r||_B = 1.821411e-06\n",
       "  7 KSP residual norm ||r||_B = 2.130719e-06\n",
       "  8 KSP residual norm ||r||_B = 2.071216e-06\n",
       "  9 KSP residual norm ||r||_B = 2.097010e-06\n",
       " 10 KSP residual norm ||r||_B = 2.382232e-06\n",
       " 11 KSP residual norm ||r||_B = 2.079427e-06\n",
       " 12 KSP residual norm ||r||_B = 1.197219e-06\n",
       " 13 KSP residual norm ||r||_B = 4.170688e-07\n",
       " 14 KSP residual norm ||r||_B = 1.470541e-07\n",
       " 15 KSP residual norm ||r||_B = 4.814647e-08\n",
       " 16 KSP residual norm ||r||_B = 1.388520e-08\n",
       " 17 KSP residual norm ||r||_B = 4.132450e-09\n",
       " 18 KSP residual norm ||r||_B = 1.009905e-09\n",
       " 19 KSP residual norm ||r||_B = 2.218670e-10\n",
       " 20 KSP residual norm ||r||_B = 4.847334e-11\n",
       " 21 KSP residual norm ||r||_B = 1.027582e-11\n",
       " 22 KSP residual norm ||r||_B = 2.112314e-12\n",
       " 23 KSP residual norm ||r||_B = 4.237828e-13\n",
       " 24 KSP residual norm ||r||_B = 9.655384e-14\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.594e-01)\n",
       " Sol. ||E|| = 6.165606e+00, ||B|| = 1.217817e-01\n",
       " Field energy E (4.618e-15 J) + H (9.420e-15 J) = 1.404e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 29\n",
       " Updating solution error estimates\n",
       "\n",
       "It 29/100: t = 1.450000e-01 ns (elapsed time = 1.30e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 5.910983e-06\n",
       "  1 KSP residual norm ||r||_B = 3.508290e-06\n",
       "  2 KSP residual norm ||r||_B = 2.435163e-06\n",
       "  3 KSP residual norm ||r||_B = 2.107683e-06\n",
       "  4 KSP residual norm ||r||_B = 1.907184e-06\n",
       "  5 KSP residual norm ||r||_B = 2.304601e-06\n",
       "  6 KSP residual norm ||r||_B = 3.491333e-06\n",
       "  7 KSP residual norm ||r||_B = 4.421985e-06\n",
       "  8 KSP residual norm ||r||_B = 3.664916e-06\n",
       "  9 KSP residual norm ||r||_B = 3.433580e-06\n",
       " 10 KSP residual norm ||r||_B = 4.199182e-06\n",
       " 11 KSP residual norm ||r||_B = 3.669164e-06\n",
       " 12 KSP residual norm ||r||_B = 2.335257e-06\n",
       " 13 KSP residual norm ||r||_B = 8.920765e-07\n",
       " 14 KSP residual norm ||r||_B = 2.981546e-07\n",
       " 15 KSP residual norm ||r||_B = 9.521662e-08\n",
       " 16 KSP residual norm ||r||_B = 2.866119e-08\n",
       " 17 KSP residual norm ||r||_B = 8.531157e-09\n",
       " 18 KSP residual norm ||r||_B = 2.123948e-09\n",
       " 19 KSP residual norm ||r||_B = 4.764796e-10\n",
       " 20 KSP residual norm ||r||_B = 1.004636e-10\n",
       " 21 KSP residual norm ||r||_B = 2.034625e-11\n",
       " 22 KSP residual norm ||r||_B = 4.274891e-12\n",
       " 23 KSP residual norm ||r||_B = 9.194968e-13\n",
       " 24 KSP residual norm ||r||_B = 2.046509e-13\n",
       " 25 KSP residual norm ||r||_B = 4.494187e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.681e-01)\n",
       " Sol. ||E|| = 7.555200e+00, ||B|| = 1.493026e-01\n",
       " Field energy E (6.934e-15 J) + H (1.416e-14 J) = 2.109e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 30/100: t = 1.500000e-01 ns (elapsed time = 1.34e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 2.581571e-06\n",
       "  1 KSP residual norm ||r||_B = 2.395551e-06\n",
       "  2 KSP residual norm ||r||_B = 3.628478e-06\n",
       "  3 KSP residual norm ||r||_B = 5.776273e-06\n",
       "  4 KSP residual norm ||r||_B = 6.868491e-06\n",
       "  5 KSP residual norm ||r||_B = 5.785782e-06\n",
       "  6 KSP residual norm ||r||_B = 5.273912e-06\n",
       "  7 KSP residual norm ||r||_B = 6.153211e-06\n",
       "  8 KSP residual norm ||r||_B = 6.170494e-06\n",
       "  9 KSP residual norm ||r||_B = 3.169788e-06\n",
       " 10 KSP residual norm ||r||_B = 1.314722e-06\n",
       " 11 KSP residual norm ||r||_B = 7.827175e-07\n",
       " 12 KSP residual norm ||r||_B = 5.833239e-07\n",
       " 13 KSP residual norm ||r||_B = 2.082360e-07\n",
       " 14 KSP residual norm ||r||_B = 4.886820e-08\n",
       " 15 KSP residual norm ||r||_B = 1.581452e-08\n",
       " 16 KSP residual norm ||r||_B = 5.805280e-09\n",
       " 17 KSP residual norm ||r||_B = 1.920298e-09\n",
       " 18 KSP residual norm ||r||_B = 5.821724e-10\n",
       " 19 KSP residual norm ||r||_B = 1.560569e-10\n",
       " 20 KSP residual norm ||r||_B = 3.617270e-11\n",
       " 21 KSP residual norm ||r||_B = 7.887924e-12\n",
       " 22 KSP residual norm ||r||_B = 1.655712e-12\n",
       " 23 KSP residual norm ||r||_B = 3.324934e-13\n",
       " 24 KSP residual norm ||r||_B = 7.447176e-14\n",
       " 25 KSP residual norm ||r||_B = 1.730579e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.528e-01)\n",
       " Sol. ||E|| = 9.037691e+00, ||B|| = 1.786846e-01\n",
       " Field energy E (9.922e-15 J) + H (2.028e-14 J) = 3.020e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 31\n",
       " Updating solution error estimates\n",
       "\n",
       "It 31/100: t = 1.550000e-01 ns (elapsed time = 1.39e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.094582e-06\n",
       "  1 KSP residual norm ||r||_B = 5.184286e-06\n",
       "  2 KSP residual norm ||r||_B = 3.992908e-06\n",
       "  3 KSP residual norm ||r||_B = 3.880615e-06\n",
       "  4 KSP residual norm ||r||_B = 4.094100e-06\n",
       "  5 KSP residual norm ||r||_B = 5.850131e-06\n",
       "  6 KSP residual norm ||r||_B = 1.005949e-05\n",
       "  7 KSP residual norm ||r||_B = 1.189025e-05\n",
       "  8 KSP residual norm ||r||_B = 6.937150e-06\n",
       "  9 KSP residual norm ||r||_B = 4.098873e-06\n",
       " 10 KSP residual norm ||r||_B = 3.876688e-06\n",
       " 11 KSP residual norm ||r||_B = 3.301243e-06\n",
       " 12 KSP residual norm ||r||_B = 2.487418e-06\n",
       " 13 KSP residual norm ||r||_B = 1.135449e-06\n",
       " 14 KSP residual norm ||r||_B = 3.758784e-07\n",
       " 15 KSP residual norm ||r||_B = 1.200943e-07\n",
       " 16 KSP residual norm ||r||_B = 3.655149e-08\n",
       " 17 KSP residual norm ||r||_B = 1.101344e-08\n",
       " 18 KSP residual norm ||r||_B = 2.841211e-09\n",
       " 19 KSP residual norm ||r||_B = 6.488956e-10\n",
       " 20 KSP residual norm ||r||_B = 1.344174e-10\n",
       " 21 KSP residual norm ||r||_B = 2.663056e-11\n",
       " 22 KSP residual norm ||r||_B = 5.629511e-12\n",
       " 23 KSP residual norm ||r||_B = 1.241969e-12\n",
       " 24 KSP residual norm ||r||_B = 2.724959e-13\n",
       " 25 KSP residual norm ||r||_B = 5.859170e-14\n",
       " 26 KSP residual norm ||r||_B = 1.291479e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.723e-01)\n",
       " Sol. ||E|| = 1.056079e+01, ||B|| = 2.088961e-01\n",
       " Field energy E (1.355e-14 J) + H (2.772e-14 J) = 4.127e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 32/100: t = 1.600000e-01 ns (elapsed time = 1.43e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 3.721863e-06\n",
       "  1 KSP residual norm ||r||_B = 4.269705e-06\n",
       "  2 KSP residual norm ||r||_B = 6.297089e-06\n",
       "  3 KSP residual norm ||r||_B = 8.315130e-06\n",
       "  4 KSP residual norm ||r||_B = 1.049541e-05\n",
       "  5 KSP residual norm ||r||_B = 1.082031e-05\n",
       "  6 KSP residual norm ||r||_B = 1.117580e-05\n",
       "  7 KSP residual norm ||r||_B = 8.068167e-06\n",
       "  8 KSP residual norm ||r||_B = 6.708477e-06\n",
       "  9 KSP residual norm ||r||_B = 5.763399e-06\n",
       " 10 KSP residual norm ||r||_B = 4.583827e-06\n",
       " 11 KSP residual norm ||r||_B = 2.775946e-06\n",
       " 12 KSP residual norm ||r||_B = 1.052611e-06\n",
       " 13 KSP residual norm ||r||_B = 3.774477e-07\n",
       " 14 KSP residual norm ||r||_B = 1.244665e-07\n",
       " 15 KSP residual norm ||r||_B = 4.285401e-08\n",
       " 16 KSP residual norm ||r||_B = 1.159853e-08\n",
       " 17 KSP residual norm ||r||_B = 2.765095e-09\n",
       " 18 KSP residual norm ||r||_B = 6.738434e-10\n",
       " 19 KSP residual norm ||r||_B = 1.802458e-10\n",
       " 20 KSP residual norm ||r||_B = 4.281894e-11\n",
       " 21 KSP residual norm ||r||_B = 8.593072e-12\n",
       " 22 KSP residual norm ||r||_B = 1.621557e-12\n",
       " 23 KSP residual norm ||r||_B = 3.247793e-13\n",
       " 24 KSP residual norm ||r||_B = 7.227571e-14\n",
       " 25 KSP residual norm ||r||_B = 1.702447e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.645e-01)\n",
       " Sol. ||E|| = 1.205822e+01, ||B|| = 2.386278e-01\n",
       " Field energy E (1.766e-14 J) + H (3.617e-14 J) = 5.383e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 33\n",
       " Updating solution error estimates\n",
       "\n",
       "It 33/100: t = 1.650000e-01 ns (elapsed time = 1.48e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.887337e-06\n",
       "  1 KSP residual norm ||r||_B = 6.616980e-06\n",
       "  2 KSP residual norm ||r||_B = 5.366985e-06\n",
       "  3 KSP residual norm ||r||_B = 5.435196e-06\n",
       "  4 KSP residual norm ||r||_B = 6.027524e-06\n",
       "  5 KSP residual norm ||r||_B = 8.995357e-06\n",
       "  6 KSP residual norm ||r||_B = 1.580079e-05\n",
       "  7 KSP residual norm ||r||_B = 1.704952e-05\n",
       "  8 KSP residual norm ||r||_B = 8.100092e-06\n",
       "  9 KSP residual norm ||r||_B = 3.127053e-06\n",
       " 10 KSP residual norm ||r||_B = 1.769129e-06\n",
       " 11 KSP residual norm ||r||_B = 1.088065e-06\n",
       " 12 KSP residual norm ||r||_B = 9.484151e-07\n",
       " 13 KSP residual norm ||r||_B = 9.156957e-07\n",
       " 14 KSP residual norm ||r||_B = 4.070149e-07\n",
       " 15 KSP residual norm ||r||_B = 1.357226e-07\n",
       " 16 KSP residual norm ||r||_B = 4.176340e-08\n",
       " 17 KSP residual norm ||r||_B = 1.274139e-08\n",
       " 18 KSP residual norm ||r||_B = 3.382569e-09\n",
       " 19 KSP residual norm ||r||_B = 7.847763e-10\n",
       " 20 KSP residual norm ||r||_B = 1.613052e-10\n",
       " 21 KSP residual norm ||r||_B = 3.152558e-11\n",
       " 22 KSP residual norm ||r||_B = 6.661336e-12\n",
       " 23 KSP residual norm ||r||_B = 1.490519e-12\n",
       " 24 KSP residual norm ||r||_B = 3.252813e-13\n",
       " 25 KSP residual norm ||r||_B = 6.916950e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.666e-01)\n",
       " Sol. ||E|| = 1.345199e+01, ||B|| = 2.663364e-01\n",
       " Field energy E (2.198e-14 J) + H (4.506e-14 J) = 6.704e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 34/100: t = 1.700000e-01 ns (elapsed time = 1.52e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 4.759530e-06\n",
       "  1 KSP residual norm ||r||_B = 5.314589e-06\n",
       "  2 KSP residual norm ||r||_B = 7.155738e-06\n",
       "  3 KSP residual norm ||r||_B = 9.175474e-06\n",
       "  4 KSP residual norm ||r||_B = 1.194806e-05\n",
       "  5 KSP residual norm ||r||_B = 1.318273e-05\n",
       "  6 KSP residual norm ||r||_B = 1.445295e-05\n",
       "  7 KSP residual norm ||r||_B = 9.893342e-06\n",
       "  8 KSP residual norm ||r||_B = 8.399870e-06\n",
       "  9 KSP residual norm ||r||_B = 7.720270e-06\n",
       " 10 KSP residual norm ||r||_B = 6.083491e-06\n",
       " 11 KSP residual norm ||r||_B = 3.555270e-06\n",
       " 12 KSP residual norm ||r||_B = 1.422327e-06\n",
       " 13 KSP residual norm ||r||_B = 5.275135e-07\n",
       " 14 KSP residual norm ||r||_B = 1.621767e-07\n",
       " 15 KSP residual norm ||r||_B = 5.428488e-08\n",
       " 16 KSP residual norm ||r||_B = 1.572942e-08\n",
       " 17 KSP residual norm ||r||_B = 3.833604e-09\n",
       " 18 KSP residual norm ||r||_B = 8.976509e-10\n",
       " 19 KSP residual norm ||r||_B = 2.318486e-10\n",
       " 20 KSP residual norm ||r||_B = 5.466728e-11\n",
       " 21 KSP residual norm ||r||_B = 1.078798e-11\n",
       " 22 KSP residual norm ||r||_B = 1.958083e-12\n",
       " 23 KSP residual norm ||r||_B = 3.808424e-13\n",
       " 24 KSP residual norm ||r||_B = 8.268626e-14\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.516e-01)\n",
       " Sol. ||E|| = 1.465613e+01, ||B|| = 2.903187e-01\n",
       " Field energy E (2.609e-14 J) + H (5.354e-14 J) = 7.963e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 35\n",
       " Updating solution error estimates\n",
       "\n",
       "It 35/100: t = 1.750000e-01 ns (elapsed time = 1.57e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.041212e-05\n",
       "  1 KSP residual norm ||r||_B = 7.030401e-06\n",
       "  2 KSP residual norm ||r||_B = 5.752212e-06\n",
       "  3 KSP residual norm ||r||_B = 5.798499e-06\n",
       "  4 KSP residual norm ||r||_B = 6.448937e-06\n",
       "  5 KSP residual norm ||r||_B = 9.652109e-06\n",
       "  6 KSP residual norm ||r||_B = 1.709247e-05\n",
       "  7 KSP residual norm ||r||_B = 1.806081e-05\n",
       "  8 KSP residual norm ||r||_B = 8.296853e-06\n",
       "  9 KSP residual norm ||r||_B = 3.138814e-06\n",
       " 10 KSP residual norm ||r||_B = 1.887703e-06\n",
       " 11 KSP residual norm ||r||_B = 1.323402e-06\n",
       " 12 KSP residual norm ||r||_B = 1.171028e-06\n",
       " 13 KSP residual norm ||r||_B = 1.024151e-06\n",
       " 14 KSP residual norm ||r||_B = 4.202012e-07\n",
       " 15 KSP residual norm ||r||_B = 1.372827e-07\n",
       " 16 KSP residual norm ||r||_B = 4.221711e-08\n",
       " 17 KSP residual norm ||r||_B = 1.297962e-08\n",
       " 18 KSP residual norm ||r||_B = 3.510946e-09\n",
       " 19 KSP residual norm ||r||_B = 8.241339e-10\n",
       " 20 KSP residual norm ||r||_B = 1.690661e-10\n",
       " 21 KSP residual norm ||r||_B = 3.279304e-11\n",
       " 22 KSP residual norm ||r||_B = 6.912240e-12\n",
       " 23 KSP residual norm ||r||_B = 1.556649e-12\n",
       " 24 KSP residual norm ||r||_B = 3.394492e-13\n",
       " 25 KSP residual norm ||r||_B = 7.179231e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.545e-01)\n",
       " Sol. ||E|| = 1.558180e+01, ||B|| = 3.088125e-01\n",
       " Field energy E (2.949e-14 J) + H (6.058e-14 J) = 9.007e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 36/100: t = 1.800000e-01 ns (elapsed time = 1.61e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 4.738248e-06\n",
       "  1 KSP residual norm ||r||_B = 4.844810e-06\n",
       "  2 KSP residual norm ||r||_B = 6.405660e-06\n",
       "  3 KSP residual norm ||r||_B = 8.275571e-06\n",
       "  4 KSP residual norm ||r||_B = 1.046462e-05\n",
       "  5 KSP residual norm ||r||_B = 1.088670e-05\n",
       "  6 KSP residual norm ||r||_B = 1.231086e-05\n",
       "  7 KSP residual norm ||r||_B = 1.046860e-05\n",
       "  8 KSP residual norm ||r||_B = 9.425911e-06\n",
       "  9 KSP residual norm ||r||_B = 8.014145e-06\n",
       " 10 KSP residual norm ||r||_B = 6.548940e-06\n",
       " 11 KSP residual norm ||r||_B = 4.028175e-06\n",
       " 12 KSP residual norm ||r||_B = 1.478523e-06\n",
       " 13 KSP residual norm ||r||_B = 5.115396e-07\n",
       " 14 KSP residual norm ||r||_B = 1.765086e-07\n",
       " 15 KSP residual norm ||r||_B = 6.140050e-08\n",
       " 16 KSP residual norm ||r||_B = 1.544729e-08\n",
       " 17 KSP residual norm ||r||_B = 3.410592e-09\n",
       " 18 KSP residual norm ||r||_B = 7.635432e-10\n",
       " 19 KSP residual norm ||r||_B = 2.038598e-10\n",
       " 20 KSP residual norm ||r||_B = 5.369513e-11\n",
       " 21 KSP residual norm ||r||_B = 1.173978e-11\n",
       " 22 KSP residual norm ||r||_B = 2.320628e-12\n",
       " 23 KSP residual norm ||r||_B = 4.790686e-13\n",
       " 24 KSP residual norm ||r||_B = 1.081911e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.457e-01)\n",
       " Sol. ||E|| = 1.614351e+01, ||B|| = 3.201191e-01\n",
       " Field energy E (3.166e-14 J) + H (6.509e-14 J) = 9.675e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 37\n",
       " Updating solution error estimates\n",
       "\n",
       "It 37/100: t = 1.850000e-01 ns (elapsed time = 1.65e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.068927e-06\n",
       "  1 KSP residual norm ||r||_B = 5.899356e-06\n",
       "  2 KSP residual norm ||r||_B = 4.625315e-06\n",
       "  3 KSP residual norm ||r||_B = 4.395998e-06\n",
       "  4 KSP residual norm ||r||_B = 4.643760e-06\n",
       "  5 KSP residual norm ||r||_B = 6.716775e-06\n",
       "  6 KSP residual norm ||r||_B = 1.211790e-05\n",
       "  7 KSP residual norm ||r||_B = 1.409647e-05\n",
       "  8 KSP residual norm ||r||_B = 7.267712e-06\n",
       "  9 KSP residual norm ||r||_B = 3.661542e-06\n",
       " 10 KSP residual norm ||r||_B = 3.430757e-06\n",
       " 11 KSP residual norm ||r||_B = 2.960906e-06\n",
       " 12 KSP residual norm ||r||_B = 2.146645e-06\n",
       " 13 KSP residual norm ||r||_B = 1.142323e-06\n",
       " 14 KSP residual norm ||r||_B = 3.815985e-07\n",
       " 15 KSP residual norm ||r||_B = 1.209532e-07\n",
       " 16 KSP residual norm ||r||_B = 3.704608e-08\n",
       " 17 KSP residual norm ||r||_B = 1.139915e-08\n",
       " 18 KSP residual norm ||r||_B = 3.091397e-09\n",
       " 19 KSP residual norm ||r||_B = 7.273042e-10\n",
       " 20 KSP residual norm ||r||_B = 1.494995e-10\n",
       " 21 KSP residual norm ||r||_B = 2.896714e-11\n",
       " 22 KSP residual norm ||r||_B = 6.096547e-12\n",
       " 23 KSP residual norm ||r||_B = 1.370213e-12\n",
       " 24 KSP residual norm ||r||_B = 2.993614e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.599e-01)\n",
       " Sol. ||E|| = 1.626591e+01, ||B|| = 3.227383e-01\n",
       " Field energy E (3.214e-14 J) + H (6.616e-14 J) = 9.830e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 38/100: t = 1.900000e-01 ns (elapsed time = 1.69e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 4.310555e-06\n",
       "  1 KSP residual norm ||r||_B = 2.979414e-06\n",
       "  2 KSP residual norm ||r||_B = 3.185659e-06\n",
       "  3 KSP residual norm ||r||_B = 4.378524e-06\n",
       "  4 KSP residual norm ||r||_B = 5.367988e-06\n",
       "  5 KSP residual norm ||r||_B = 4.950396e-06\n",
       "  6 KSP residual norm ||r||_B = 4.857883e-06\n",
       "  7 KSP residual norm ||r||_B = 6.762765e-06\n",
       "  8 KSP residual norm ||r||_B = 9.427331e-06\n",
       "  9 KSP residual norm ||r||_B = 5.795660e-06\n",
       " 10 KSP residual norm ||r||_B = 2.248639e-06\n",
       " 11 KSP residual norm ||r||_B = 1.113647e-06\n",
       " 12 KSP residual norm ||r||_B = 8.865306e-07\n",
       " 13 KSP residual norm ||r||_B = 3.875217e-07\n",
       " 14 KSP residual norm ||r||_B = 9.469058e-08\n",
       " 15 KSP residual norm ||r||_B = 2.792556e-08\n",
       " 16 KSP residual norm ||r||_B = 8.665806e-09\n",
       " 17 KSP residual norm ||r||_B = 2.993456e-09\n",
       " 18 KSP residual norm ||r||_B = 1.085355e-09\n",
       " 19 KSP residual norm ||r||_B = 3.072978e-10\n",
       " 20 KSP residual norm ||r||_B = 7.047460e-11\n",
       " 21 KSP residual norm ||r||_B = 1.525222e-11\n",
       " 22 KSP residual norm ||r||_B = 3.186748e-12\n",
       " 23 KSP residual norm ||r||_B = 6.371363e-13\n",
       " 24 KSP residual norm ||r||_B = 1.430451e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.459e-01)\n",
       " Sol. ||E|| = 1.589066e+01, ||B|| = 3.155039e-01\n",
       " Field energy E (3.067e-14 J) + H (6.323e-14 J) = 9.390e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 39\n",
       " Updating solution error estimates\n",
       "\n",
       "It 39/100: t = 1.950000e-01 ns (elapsed time = 1.74e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 5.997301e-06\n",
       "  1 KSP residual norm ||r||_B = 3.397447e-06\n",
       "  2 KSP residual norm ||r||_B = 2.239469e-06\n",
       "  3 KSP residual norm ||r||_B = 1.663785e-06\n",
       "  4 KSP residual norm ||r||_B = 1.272615e-06\n",
       "  5 KSP residual norm ||r||_B = 1.358992e-06\n",
       "  6 KSP residual norm ||r||_B = 2.257682e-06\n",
       "  7 KSP residual norm ||r||_B = 3.708166e-06\n",
       "  8 KSP residual norm ||r||_B = 3.135538e-06\n",
       "  9 KSP residual norm ||r||_B = 2.257141e-06\n",
       " 10 KSP residual norm ||r||_B = 2.615070e-06\n",
       " 11 KSP residual norm ||r||_B = 2.432071e-06\n",
       " 12 KSP residual norm ||r||_B = 1.794626e-06\n",
       " 13 KSP residual norm ||r||_B = 8.457954e-07\n",
       " 14 KSP residual norm ||r||_B = 2.781332e-07\n",
       " 15 KSP residual norm ||r||_B = 8.916148e-08\n",
       " 16 KSP residual norm ||r||_B = 2.710063e-08\n",
       " 17 KSP residual norm ||r||_B = 8.232607e-09\n",
       " 18 KSP residual norm ||r||_B = 2.164578e-09\n",
       " 19 KSP residual norm ||r||_B = 4.994289e-10\n",
       " 20 KSP residual norm ||r||_B = 1.038687e-10\n",
       " 21 KSP residual norm ||r||_B = 2.043685e-11\n",
       " 22 KSP residual norm ||r||_B = 4.307171e-12\n",
       " 23 KSP residual norm ||r||_B = 9.471834e-13\n",
       " 24 KSP residual norm ||r||_B = 2.085254e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.505e-01)\n",
       " Sol. ||E|| = 1.498253e+01, ||B|| = 2.977073e-01\n",
       " Field energy E (2.727e-14 J) + H (5.630e-14 J) = 8.357e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 40/100: t = 2.000000e-01 ns (elapsed time = 1.78e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.210022e-06\n",
       "  1 KSP residual norm ||r||_B = 3.175666e-06\n",
       "  2 KSP residual norm ||r||_B = 1.856463e-06\n",
       "  3 KSP residual norm ||r||_B = 1.349888e-06\n",
       "  4 KSP residual norm ||r||_B = 9.578383e-07\n",
       "  5 KSP residual norm ||r||_B = 7.314016e-07\n",
       "  6 KSP residual norm ||r||_B = 6.296777e-07\n",
       "  7 KSP residual norm ||r||_B = 6.039891e-07\n",
       "  8 KSP residual norm ||r||_B = 5.483443e-07\n",
       "  9 KSP residual norm ||r||_B = 4.998174e-07\n",
       " 10 KSP residual norm ||r||_B = 6.776331e-07\n",
       " 11 KSP residual norm ||r||_B = 1.100882e-06\n",
       " 12 KSP residual norm ||r||_B = 1.629992e-06\n",
       " 13 KSP residual norm ||r||_B = 8.812036e-07\n",
       " 14 KSP residual norm ||r||_B = 3.267692e-07\n",
       " 15 KSP residual norm ||r||_B = 1.080126e-07\n",
       " 16 KSP residual norm ||r||_B = 3.208170e-08\n",
       " 17 KSP residual norm ||r||_B = 9.563254e-09\n",
       " 18 KSP residual norm ||r||_B = 2.310868e-09\n",
       " 19 KSP residual norm ||r||_B = 5.045364e-10\n",
       " 20 KSP residual norm ||r||_B = 1.097130e-10\n",
       " 21 KSP residual norm ||r||_B = 2.323094e-11\n",
       " 22 KSP residual norm ||r||_B = 4.799124e-12\n",
       " 23 KSP residual norm ||r||_B = 9.671143e-13\n",
       " 24 KSP residual norm ||r||_B = 2.200371e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.534e-01)\n",
       " Sol. ||E|| = 1.353436e+01, ||B|| = 2.691937e-01\n",
       " Field energy E (2.225e-14 J) + H (4.603e-14 J) = 6.828e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 41\n",
       " Updating solution error estimates\n",
       "\n",
       "It 41/100: t = 2.050000e-01 ns (elapsed time = 1.83e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 3.173132e-06\n",
       "  1 KSP residual norm ||r||_B = 2.042747e-06\n",
       "  2 KSP residual norm ||r||_B = 2.457153e-06\n",
       "  3 KSP residual norm ||r||_B = 4.184471e-06\n",
       "  4 KSP residual norm ||r||_B = 6.703950e-06\n",
       "  5 KSP residual norm ||r||_B = 7.542140e-06\n",
       "  6 KSP residual norm ||r||_B = 5.900188e-06\n",
       "  7 KSP residual norm ||r||_B = 4.139652e-06\n",
       "  8 KSP residual norm ||r||_B = 3.013065e-06\n",
       "  9 KSP residual norm ||r||_B = 1.826087e-06\n",
       " 10 KSP residual norm ||r||_B = 1.223409e-06\n",
       " 11 KSP residual norm ||r||_B = 1.028815e-06\n",
       " 12 KSP residual norm ||r||_B = 9.067554e-07\n",
       " 13 KSP residual norm ||r||_B = 3.872995e-07\n",
       " 14 KSP residual norm ||r||_B = 1.349205e-07\n",
       " 15 KSP residual norm ||r||_B = 4.966274e-08\n",
       " 16 KSP residual norm ||r||_B = 1.437767e-08\n",
       " 17 KSP residual norm ||r||_B = 4.322457e-09\n",
       " 18 KSP residual norm ||r||_B = 1.119367e-09\n",
       " 19 KSP residual norm ||r||_B = 2.465284e-10\n",
       " 20 KSP residual norm ||r||_B = 5.356225e-11\n",
       " 21 KSP residual norm ||r||_B = 1.170302e-11\n",
       " 22 KSP residual norm ||r||_B = 2.453319e-12\n",
       " 23 KSP residual norm ||r||_B = 4.685249e-13\n",
       " 24 KSP residual norm ||r||_B = 1.017524e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.388e-01)\n",
       " Sol. ||E|| = 1.156989e+01, ||B|| = 2.304214e-01\n",
       " Field energy E (1.626e-14 J) + H (3.373e-14 J) = 4.999e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 42/100: t = 2.100000e-01 ns (elapsed time = 1.86e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.010113e-05\n",
       "  1 KSP residual norm ||r||_B = 6.157453e-06\n",
       "  2 KSP residual norm ||r||_B = 4.665691e-06\n",
       "  3 KSP residual norm ||r||_B = 4.600371e-06\n",
       "  4 KSP residual norm ||r||_B = 4.901035e-06\n",
       "  5 KSP residual norm ||r||_B = 6.940281e-06\n",
       "  6 KSP residual norm ||r||_B = 1.170365e-05\n",
       "  7 KSP residual norm ||r||_B = 1.457668e-05\n",
       "  8 KSP residual norm ||r||_B = 8.976251e-06\n",
       "  9 KSP residual norm ||r||_B = 4.631177e-06\n",
       " 10 KSP residual norm ||r||_B = 3.489847e-06\n",
       " 11 KSP residual norm ||r||_B = 2.943032e-06\n",
       " 12 KSP residual norm ||r||_B = 2.715969e-06\n",
       " 13 KSP residual norm ||r||_B = 1.416477e-06\n",
       " 14 KSP residual norm ||r||_B = 4.895035e-07\n",
       " 15 KSP residual norm ||r||_B = 1.580779e-07\n",
       " 16 KSP residual norm ||r||_B = 4.799215e-08\n",
       " 17 KSP residual norm ||r||_B = 1.438561e-08\n",
       " 18 KSP residual norm ||r||_B = 3.645966e-09\n",
       " 19 KSP residual norm ||r||_B = 8.241016e-10\n",
       " 20 KSP residual norm ||r||_B = 1.722783e-10\n",
       " 21 KSP residual norm ||r||_B = 3.459439e-11\n",
       " 22 KSP residual norm ||r||_B = 7.297537e-12\n",
       " 23 KSP residual norm ||r||_B = 1.581341e-12\n",
       " 24 KSP residual norm ||r||_B = 3.492303e-13\n",
       " 25 KSP residual norm ||r||_B = 7.612961e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.526e-01)\n",
       " Sol. ||E|| = 9.144331e+00, ||B|| = 1.824729e-01\n",
       " Field energy E (1.016e-14 J) + H (2.115e-14 J) = 3.131e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 43\n",
       " Updating solution error estimates\n",
       "\n",
       "It 43/100: t = 2.150000e-01 ns (elapsed time = 1.91e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 5.045291e-06\n",
       "  1 KSP residual norm ||r||_B = 5.707437e-06\n",
       "  2 KSP residual norm ||r||_B = 8.097662e-06\n",
       "  3 KSP residual norm ||r||_B = 1.088174e-05\n",
       "  4 KSP residual norm ||r||_B = 1.529035e-05\n",
       "  5 KSP residual norm ||r||_B = 1.739838e-05\n",
       "  6 KSP residual norm ||r||_B = 1.728970e-05\n",
       "  7 KSP residual norm ||r||_B = 8.642821e-06\n",
       "  8 KSP residual norm ||r||_B = 4.425341e-06\n",
       "  9 KSP residual norm ||r||_B = 2.919391e-06\n",
       " 10 KSP residual norm ||r||_B = 2.313856e-06\n",
       " 11 KSP residual norm ||r||_B = 2.253589e-06\n",
       " 12 KSP residual norm ||r||_B = 1.292885e-06\n",
       " 13 KSP residual norm ||r||_B = 5.355792e-07\n",
       " 14 KSP residual norm ||r||_B = 1.647923e-07\n",
       " 15 KSP residual norm ||r||_B = 5.463677e-08\n",
       " 16 KSP residual norm ||r||_B = 1.609808e-08\n",
       " 17 KSP residual norm ||r||_B = 3.960992e-09\n",
       " 18 KSP residual norm ||r||_B = 9.170182e-10\n",
       " 19 KSP residual norm ||r||_B = 2.332696e-10\n",
       " 20 KSP residual norm ||r||_B = 5.606073e-11\n",
       " 21 KSP residual norm ||r||_B = 1.130381e-11\n",
       " 22 KSP residual norm ||r||_B = 2.079160e-12\n",
       " 23 KSP residual norm ||r||_B = 3.968593e-13\n",
       " 24 KSP residual norm ||r||_B = 8.407945e-14\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.422e-01)\n",
       " Sol. ||E|| = 6.342347e+00, ||B|| = 1.270158e-01\n",
       " Field energy E (4.886e-15 J) + H (1.025e-14 J) = 1.513e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 44/100: t = 2.200000e-01 ns (elapsed time = 1.95e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.352800e-05\n",
       "  1 KSP residual norm ||r||_B = 9.048343e-06\n",
       "  2 KSP residual norm ||r||_B = 7.605490e-06\n",
       "  3 KSP residual norm ||r||_B = 8.069482e-06\n",
       "  4 KSP residual norm ||r||_B = 9.214505e-06\n",
       "  5 KSP residual norm ||r||_B = 1.383284e-05\n",
       "  6 KSP residual norm ||r||_B = 2.343161e-05\n",
       "  7 KSP residual norm ||r||_B = 2.395996e-05\n",
       "  8 KSP residual norm ||r||_B = 1.132003e-05\n",
       "  9 KSP residual norm ||r||_B = 4.362752e-06\n",
       " 10 KSP residual norm ||r||_B = 2.370717e-06\n",
       " 11 KSP residual norm ||r||_B = 1.350844e-06\n",
       " 12 KSP residual norm ||r||_B = 1.123775e-06\n",
       " 13 KSP residual norm ||r||_B = 1.162016e-06\n",
       " 14 KSP residual norm ||r||_B = 5.537717e-07\n",
       " 15 KSP residual norm ||r||_B = 1.876317e-07\n",
       " 16 KSP residual norm ||r||_B = 5.789236e-08\n",
       " 17 KSP residual norm ||r||_B = 1.764903e-08\n",
       " 18 KSP residual norm ||r||_B = 4.671827e-09\n",
       " 19 KSP residual norm ||r||_B = 1.081800e-09\n",
       " 20 KSP residual norm ||r||_B = 2.226818e-10\n",
       " 21 KSP residual norm ||r||_B = 4.366242e-11\n",
       " 22 KSP residual norm ||r||_B = 9.228551e-12\n",
       " 23 KSP residual norm ||r||_B = 2.054468e-12\n",
       " 24 KSP residual norm ||r||_B = 4.488142e-13\n",
       " 25 KSP residual norm ||r||_B = 9.577342e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.696e-01)\n",
       " Sol. ||E|| = 3.273573e+00, ||B|| = 6.621314e-02\n",
       " Field energy E (1.302e-15 J) + H (2.785e-15 J) = 4.087e-15 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 45\n",
       " Updating solution error estimates\n",
       "\n",
       "It 45/100: t = 2.250000e-01 ns (elapsed time = 2.00e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.520145e-06\n",
       "  1 KSP residual norm ||r||_B = 8.125689e-06\n",
       "  2 KSP residual norm ||r||_B = 9.935181e-06\n",
       "  3 KSP residual norm ||r||_B = 1.272282e-05\n",
       "  4 KSP residual norm ||r||_B = 1.781359e-05\n",
       "  5 KSP residual norm ||r||_B = 2.252377e-05\n",
       "  6 KSP residual norm ||r||_B = 2.578340e-05\n",
       "  7 KSP residual norm ||r||_B = 1.345490e-05\n",
       "  8 KSP residual norm ||r||_B = 8.105350e-06\n",
       "  9 KSP residual norm ||r||_B = 7.225725e-06\n",
       " 10 KSP residual norm ||r||_B = 6.434410e-06\n",
       " 11 KSP residual norm ||r||_B = 4.391308e-06\n",
       " 12 KSP residual norm ||r||_B = 2.211602e-06\n",
       " 13 KSP residual norm ||r||_B = 8.591272e-07\n",
       " 14 KSP residual norm ||r||_B = 2.322752e-07\n",
       " 15 KSP residual norm ||r||_B = 7.538796e-08\n",
       " 16 KSP residual norm ||r||_B = 2.477312e-08\n",
       " 17 KSP residual norm ||r||_B = 6.126348e-09\n",
       " 18 KSP residual norm ||r||_B = 1.290651e-09\n",
       " 19 KSP residual norm ||r||_B = 3.093915e-10\n",
       " 20 KSP residual norm ||r||_B = 7.694163e-11\n",
       " 21 KSP residual norm ||r||_B = 1.597763e-11\n",
       " 22 KSP residual norm ||r||_B = 2.862917e-12\n",
       " 23 KSP residual norm ||r||_B = 5.530964e-13\n",
       " 24 KSP residual norm ||r||_B = 1.222158e-13\n",
       " 25 KSP residual norm ||r||_B = 3.091872e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.595e-01)\n",
       " Sol. ||E|| = 9.801112e-02, ||B|| = 2.679091e-03\n",
       " Field energy E (1.141e-18 J) + H (4.587e-18 J) = 5.729e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 46/100: t = 2.300000e-01 ns (elapsed time = 2.04e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.487787e-05\n",
       "  1 KSP residual norm ||r||_B = 1.024165e-05\n",
       "  2 KSP residual norm ||r||_B = 8.855267e-06\n",
       "  3 KSP residual norm ||r||_B = 9.458663e-06\n",
       "  4 KSP residual norm ||r||_B = 1.089146e-05\n",
       "  5 KSP residual norm ||r||_B = 1.635627e-05\n",
       "  6 KSP residual norm ||r||_B = 2.728114e-05\n",
       "  7 KSP residual norm ||r||_B = 2.602717e-05\n",
       "  8 KSP residual norm ||r||_B = 1.246412e-05\n",
       "  9 KSP residual norm ||r||_B = 6.551607e-06\n",
       " 10 KSP residual norm ||r||_B = 6.397633e-06\n",
       " 11 KSP residual norm ||r||_B = 5.352230e-06\n",
       " 12 KSP residual norm ||r||_B = 3.695065e-06\n",
       " 13 KSP residual norm ||r||_B = 1.886520e-06\n",
       " 14 KSP residual norm ||r||_B = 6.179402e-07\n",
       " 15 KSP residual norm ||r||_B = 1.947335e-07\n",
       " 16 KSP residual norm ||r||_B = 5.970455e-08\n",
       " 17 KSP residual norm ||r||_B = 1.838898e-08\n",
       " 18 KSP residual norm ||r||_B = 4.999865e-09\n",
       " 19 KSP residual norm ||r||_B = 1.177594e-09\n",
       " 20 KSP residual norm ||r||_B = 2.415878e-10\n",
       " 21 KSP residual norm ||r||_B = 4.685475e-11\n",
       " 22 KSP residual norm ||r||_B = 9.872844e-12\n",
       " 23 KSP residual norm ||r||_B = 2.221180e-12\n",
       " 24 KSP residual norm ||r||_B = 4.844295e-13\n",
       " 25 KSP residual norm ||r||_B = 1.025254e-13\n",
       " 26 KSP residual norm ||r||_B = 2.273877e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.658e-01)\n",
       " Sol. ||E|| = 3.148514e+00, ||B|| = 6.116379e-02\n",
       " Field energy E (1.204e-15 J) + H (2.376e-15 J) = 3.580e-15 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 47\n",
       " Updating solution error estimates\n",
       "\n",
       "It 47/100: t = 2.350000e-01 ns (elapsed time = 2.09e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.936018e-06\n",
       "  1 KSP residual norm ||r||_B = 8.184494e-06\n",
       "  2 KSP residual norm ||r||_B = 9.740338e-06\n",
       "  3 KSP residual norm ||r||_B = 1.220256e-05\n",
       "  4 KSP residual norm ||r||_B = 1.697757e-05\n",
       "  5 KSP residual norm ||r||_B = 2.094868e-05\n",
       "  6 KSP residual norm ||r||_B = 2.505281e-05\n",
       "  7 KSP residual norm ||r||_B = 1.493547e-05\n",
       "  8 KSP residual norm ||r||_B = 1.064652e-05\n",
       "  9 KSP residual norm ||r||_B = 9.905268e-06\n",
       " 10 KSP residual norm ||r||_B = 8.478152e-06\n",
       " 11 KSP residual norm ||r||_B = 5.626332e-06\n",
       " 12 KSP residual norm ||r||_B = 2.500590e-06\n",
       " 13 KSP residual norm ||r||_B = 9.446554e-07\n",
       " 14 KSP residual norm ||r||_B = 2.729012e-07\n",
       " 15 KSP residual norm ||r||_B = 8.964671e-08\n",
       " 16 KSP residual norm ||r||_B = 2.752465e-08\n",
       " 17 KSP residual norm ||r||_B = 6.722322e-09\n",
       " 18 KSP residual norm ||r||_B = 1.470249e-09\n",
       " 19 KSP residual norm ||r||_B = 3.650006e-10\n",
       " 20 KSP residual norm ||r||_B = 8.955154e-11\n",
       " 21 KSP residual norm ||r||_B = 1.814731e-11\n",
       " 22 KSP residual norm ||r||_B = 3.246540e-12\n",
       " 23 KSP residual norm ||r||_B = 6.167002e-13\n",
       " 24 KSP residual norm ||r||_B = 1.311481e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.637e-01)\n",
       " Sol. ||E|| = 6.225179e+00, ||B|| = 1.222886e-01\n",
       " Field energy E (4.707e-15 J) + H (9.499e-15 J) = 1.421e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 48/100: t = 2.400000e-01 ns (elapsed time = 2.13e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.356240e-05\n",
       "  1 KSP residual norm ||r||_B = 9.165841e-06\n",
       "  2 KSP residual norm ||r||_B = 7.821899e-06\n",
       "  3 KSP residual norm ||r||_B = 8.153544e-06\n",
       "  4 KSP residual norm ||r||_B = 9.176914e-06\n",
       "  5 KSP residual norm ||r||_B = 1.348199e-05\n",
       "  6 KSP residual norm ||r||_B = 2.235085e-05\n",
       "  7 KSP residual norm ||r||_B = 2.188768e-05\n",
       "  8 KSP residual norm ||r||_B = 1.176298e-05\n",
       "  9 KSP residual norm ||r||_B = 8.127499e-06\n",
       " 10 KSP residual norm ||r||_B = 9.358221e-06\n",
       " 11 KSP residual norm ||r||_B = 6.541025e-06\n",
       " 12 KSP residual norm ||r||_B = 3.716376e-06\n",
       " 13 KSP residual norm ||r||_B = 1.744887e-06\n",
       " 14 KSP residual norm ||r||_B = 5.610961e-07\n",
       " 15 KSP residual norm ||r||_B = 1.760050e-07\n",
       " 16 KSP residual norm ||r||_B = 5.393011e-08\n",
       " 17 KSP residual norm ||r||_B = 1.666696e-08\n",
       " 18 KSP residual norm ||r||_B = 4.566836e-09\n",
       " 19 KSP residual norm ||r||_B = 1.081849e-09\n",
       " 20 KSP residual norm ||r||_B = 2.222306e-10\n",
       " 21 KSP residual norm ||r||_B = 4.299022e-11\n",
       " 22 KSP residual norm ||r||_B = 9.040490e-12\n",
       " 23 KSP residual norm ||r||_B = 2.034156e-12\n",
       " 24 KSP residual norm ||r||_B = 4.442591e-13\n",
       " 25 KSP residual norm ||r||_B = 9.392182e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.591e-01)\n",
       " Sol. ||E|| = 9.039740e+00, ||B|| = 1.782585e-01\n",
       " Field energy E (9.926e-15 J) + H (2.018e-14 J) = 3.011e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 49\n",
       " Updating solution error estimates\n",
       "\n",
       "It 49/100: t = 2.450000e-01 ns (elapsed time = 2.17e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.529657e-06\n",
       "  1 KSP residual norm ||r||_B = 5.826836e-06\n",
       "  2 KSP residual norm ||r||_B = 6.975133e-06\n",
       "  3 KSP residual norm ||r||_B = 8.951308e-06\n",
       "  4 KSP residual norm ||r||_B = 1.228411e-05\n",
       "  5 KSP residual norm ||r||_B = 1.376079e-05\n",
       "  6 KSP residual norm ||r||_B = 1.587656e-05\n",
       "  7 KSP residual norm ||r||_B = 1.299624e-05\n",
       "  8 KSP residual norm ||r||_B = 1.067077e-05\n",
       "  9 KSP residual norm ||r||_B = 8.996541e-06\n",
       " 10 KSP residual norm ||r||_B = 8.034047e-06\n",
       " 11 KSP residual norm ||r||_B = 5.740662e-06\n",
       " 12 KSP residual norm ||r||_B = 2.214675e-06\n",
       " 13 KSP residual norm ||r||_B = 7.655252e-07\n",
       " 14 KSP residual norm ||r||_B = 2.678175e-07\n",
       " 15 KSP residual norm ||r||_B = 9.300204e-08\n",
       " 16 KSP residual norm ||r||_B = 2.255833e-08\n",
       " 17 KSP residual norm ||r||_B = 4.725007e-09\n",
       " 18 KSP residual norm ||r||_B = 9.275048e-10\n",
       " 19 KSP residual norm ||r||_B = 2.000648e-10\n",
       " 20 KSP residual norm ||r||_B = 4.957573e-11\n",
       " 21 KSP residual norm ||r||_B = 1.326661e-11\n",
       " 22 KSP residual norm ||r||_B = 3.109901e-12\n",
       " 23 KSP residual norm ||r||_B = 6.870385e-13\n",
       " 24 KSP residual norm ||r||_B = 1.596108e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.523e-01)\n",
       " Sol. ||E|| = 1.148172e+01, ||B|| = 2.268760e-01\n",
       " Field energy E (1.601e-14 J) + H (3.270e-14 J) = 4.871e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 50/100: t = 2.500000e-01 ns (elapsed time = 2.21e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.012228e-05\n",
       "  1 KSP residual norm ||r||_B = 6.258241e-06\n",
       "  2 KSP residual norm ||r||_B = 4.948945e-06\n",
       "  3 KSP residual norm ||r||_B = 4.772964e-06\n",
       "  4 KSP residual norm ||r||_B = 4.938496e-06\n",
       "  5 KSP residual norm ||r||_B = 6.744266e-06\n",
       "  6 KSP residual norm ||r||_B = 1.107635e-05\n",
       "  7 KSP residual norm ||r||_B = 1.246086e-05\n",
       "  8 KSP residual norm ||r||_B = 8.242012e-06\n",
       "  9 KSP residual norm ||r||_B = 6.869401e-06\n",
       " 10 KSP residual norm ||r||_B = 8.264296e-06\n",
       " 11 KSP residual norm ||r||_B = 5.653810e-06\n",
       " 12 KSP residual norm ||r||_B = 3.209172e-06\n",
       " 13 KSP residual norm ||r||_B = 1.407031e-06\n",
       " 14 KSP residual norm ||r||_B = 4.476801e-07\n",
       " 15 KSP residual norm ||r||_B = 1.417830e-07\n",
       " 16 KSP residual norm ||r||_B = 4.338972e-08\n",
       " 17 KSP residual norm ||r||_B = 1.331340e-08\n",
       " 18 KSP residual norm ||r||_B = 3.573825e-09\n",
       " 19 KSP residual norm ||r||_B = 8.355181e-10\n",
       " 20 KSP residual norm ||r||_B = 1.726990e-10\n",
       " 21 KSP residual norm ||r||_B = 3.371742e-11\n",
       " 22 KSP residual norm ||r||_B = 7.100335e-12\n",
       " 23 KSP residual norm ||r||_B = 1.574847e-12\n",
       " 24 KSP residual norm ||r||_B = 3.452877e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.617e-01)\n",
       " Sol. ||E|| = 1.346537e+01, ||B|| = 2.664298e-01\n",
       " Field energy E (2.202e-14 J) + H (4.509e-14 J) = 6.711e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 51\n",
       " Updating solution error estimates\n",
       "\n",
       "It 51/100: t = 2.550000e-01 ns (elapsed time = 2.26e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 5.809901e-06\n",
       "  1 KSP residual norm ||r||_B = 3.061312e-06\n",
       "  2 KSP residual norm ||r||_B = 2.395578e-06\n",
       "  3 KSP residual norm ||r||_B = 2.918954e-06\n",
       "  4 KSP residual norm ||r||_B = 4.247063e-06\n",
       "  5 KSP residual norm ||r||_B = 4.919539e-06\n",
       "  6 KSP residual norm ||r||_B = 4.160865e-06\n",
       "  7 KSP residual norm ||r||_B = 4.462942e-06\n",
       "  8 KSP residual norm ||r||_B = 7.196234e-06\n",
       "  9 KSP residual norm ||r||_B = 6.811782e-06\n",
       " 10 KSP residual norm ||r||_B = 2.838200e-06\n",
       " 11 KSP residual norm ||r||_B = 8.962718e-07\n",
       " 12 KSP residual norm ||r||_B = 4.739492e-07\n",
       " 13 KSP residual norm ||r||_B = 3.758862e-07\n",
       " 14 KSP residual norm ||r||_B = 1.471717e-07\n",
       " 15 KSP residual norm ||r||_B = 5.295559e-08\n",
       " 16 KSP residual norm ||r||_B = 1.794261e-08\n",
       " 17 KSP residual norm ||r||_B = 6.443343e-09\n",
       " 18 KSP residual norm ||r||_B = 1.985810e-09\n",
       " 19 KSP residual norm ||r||_B = 4.705956e-10\n",
       " 20 KSP residual norm ||r||_B = 1.032862e-10\n",
       " 21 KSP residual norm ||r||_B = 2.248797e-11\n",
       " 22 KSP residual norm ||r||_B = 4.707924e-12\n",
       " 23 KSP residual norm ||r||_B = 9.140451e-13\n",
       " 24 KSP residual norm ||r||_B = 2.026241e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.520e-01)\n",
       " Sol. ||E|| = 1.493428e+01, ||B|| = 2.957885e-01\n",
       " Field energy E (2.709e-14 J) + H (5.557e-14 J) = 8.267e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 52/100: t = 2.600000e-01 ns (elapsed time = 2.29e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.193902e-06\n",
       "  1 KSP residual norm ||r||_B = 3.013303e-06\n",
       "  2 KSP residual norm ||r||_B = 1.818921e-06\n",
       "  3 KSP residual norm ||r||_B = 1.300045e-06\n",
       "  4 KSP residual norm ||r||_B = 8.798888e-07\n",
       "  5 KSP residual norm ||r||_B = 6.563881e-07\n",
       "  6 KSP residual norm ||r||_B = 6.493835e-07\n",
       "  7 KSP residual norm ||r||_B = 7.253972e-07\n",
       "  8 KSP residual norm ||r||_B = 6.705375e-07\n",
       "  9 KSP residual norm ||r||_B = 6.172134e-07\n",
       " 10 KSP residual norm ||r||_B = 9.183493e-07\n",
       " 11 KSP residual norm ||r||_B = 1.367464e-06\n",
       " 12 KSP residual norm ||r||_B = 1.672824e-06\n",
       " 13 KSP residual norm ||r||_B = 9.086383e-07\n",
       " 14 KSP residual norm ||r||_B = 3.132845e-07\n",
       " 15 KSP residual norm ||r||_B = 1.032453e-07\n",
       " 16 KSP residual norm ||r||_B = 3.101735e-08\n",
       " 17 KSP residual norm ||r||_B = 9.372396e-09\n",
       " 18 KSP residual norm ||r||_B = 2.380703e-09\n",
       " 19 KSP residual norm ||r||_B = 5.339105e-10\n",
       " 20 KSP residual norm ||r||_B = 1.133635e-10\n",
       " 21 KSP residual norm ||r||_B = 2.312333e-11\n",
       " 22 KSP residual norm ||r||_B = 4.872238e-12\n",
       " 23 KSP residual norm ||r||_B = 1.022645e-12\n",
       " 24 KSP residual norm ||r||_B = 2.270008e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.520e-01)\n",
       " Sol. ||E|| = 1.586347e+01, ||B|| = 3.144434e-01\n",
       " Field energy E (3.057e-14 J) + H (6.281e-14 J) = 9.337e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 53\n",
       " Updating solution error estimates\n",
       "\n",
       "It 53/100: t = 2.650000e-01 ns (elapsed time = 2.34e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.955117e-06\n",
       "  1 KSP residual norm ||r||_B = 3.805084e-06\n",
       "  2 KSP residual norm ||r||_B = 2.131062e-06\n",
       "  3 KSP residual norm ||r||_B = 1.579657e-06\n",
       "  4 KSP residual norm ||r||_B = 1.330172e-06\n",
       "  5 KSP residual norm ||r||_B = 1.406445e-06\n",
       "  6 KSP residual norm ||r||_B = 1.858021e-06\n",
       "  7 KSP residual norm ||r||_B = 2.768834e-06\n",
       "  8 KSP residual norm ||r||_B = 3.482316e-06\n",
       "  9 KSP residual norm ||r||_B = 2.731334e-06\n",
       " 10 KSP residual norm ||r||_B = 2.286468e-06\n",
       " 11 KSP residual norm ||r||_B = 2.305225e-06\n",
       " 12 KSP residual norm ||r||_B = 2.404950e-06\n",
       " 13 KSP residual norm ||r||_B = 1.152060e-06\n",
       " 14 KSP residual norm ||r||_B = 4.132958e-07\n",
       " 15 KSP residual norm ||r||_B = 1.385434e-07\n",
       " 16 KSP residual norm ||r||_B = 4.153954e-08\n",
       " 17 KSP residual norm ||r||_B = 1.251408e-08\n",
       " 18 KSP residual norm ||r||_B = 3.058494e-09\n",
       " 19 KSP residual norm ||r||_B = 6.682811e-10\n",
       " 20 KSP residual norm ||r||_B = 1.445928e-10\n",
       " 21 KSP residual norm ||r||_B = 3.058179e-11\n",
       " 22 KSP residual norm ||r||_B = 6.363960e-12\n",
       " 23 KSP residual norm ||r||_B = 1.281473e-12\n",
       " 24 KSP residual norm ||r||_B = 2.884298e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.590e-01)\n",
       " Sol. ||E|| = 1.625896e+01, ||B|| = 3.225020e-01\n",
       " Field energy E (3.211e-14 J) + H (6.607e-14 J) = 9.818e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 54/100: t = 2.700000e-01 ns (elapsed time = 2.38e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 4.529593e-06\n",
       "  1 KSP residual norm ||r||_B = 2.550809e-06\n",
       "  2 KSP residual norm ||r||_B = 2.678979e-06\n",
       "  3 KSP residual norm ||r||_B = 4.250662e-06\n",
       "  4 KSP residual norm ||r||_B = 7.488221e-06\n",
       "  5 KSP residual norm ||r||_B = 9.720117e-06\n",
       "  6 KSP residual norm ||r||_B = 6.749183e-06\n",
       "  7 KSP residual norm ||r||_B = 3.953865e-06\n",
       "  8 KSP residual norm ||r||_B = 3.701339e-06\n",
       "  9 KSP residual norm ||r||_B = 3.429955e-06\n",
       " 10 KSP residual norm ||r||_B = 1.983299e-06\n",
       " 11 KSP residual norm ||r||_B = 1.111936e-06\n",
       " 12 KSP residual norm ||r||_B = 9.206357e-07\n",
       " 13 KSP residual norm ||r||_B = 4.486083e-07\n",
       " 14 KSP residual norm ||r||_B = 1.238104e-07\n",
       " 15 KSP residual norm ||r||_B = 4.247286e-08\n",
       " 16 KSP residual norm ||r||_B = 1.426590e-08\n",
       " 17 KSP residual norm ||r||_B = 5.031997e-09\n",
       " 18 KSP residual norm ||r||_B = 1.545304e-09\n",
       " 19 KSP residual norm ||r||_B = 3.620135e-10\n",
       " 20 KSP residual norm ||r||_B = 7.874170e-11\n",
       " 21 KSP residual norm ||r||_B = 1.729884e-11\n",
       " 22 KSP residual norm ||r||_B = 3.680940e-12\n",
       " 23 KSP residual norm ||r||_B = 6.996181e-13\n",
       " 24 KSP residual norm ||r||_B = 1.492688e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.465e-01)\n",
       " Sol. ||E|| = 1.615493e+01, ||B|| = 3.206318e-01\n",
       " Field energy E (3.170e-14 J) + H (6.530e-14 J) = 9.701e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 55\n",
       " Updating solution error estimates\n",
       "\n",
       "It 55/100: t = 2.750000e-01 ns (elapsed time = 2.42e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.061030e-05\n",
       "  1 KSP residual norm ||r||_B = 5.945457e-06\n",
       "  2 KSP residual norm ||r||_B = 4.373313e-06\n",
       "  3 KSP residual norm ||r||_B = 4.388278e-06\n",
       "  4 KSP residual norm ||r||_B = 4.785009e-06\n",
       "  5 KSP residual norm ||r||_B = 6.641040e-06\n",
       "  6 KSP residual norm ||r||_B = 1.090823e-05\n",
       "  7 KSP residual norm ||r||_B = 1.437356e-05\n",
       "  8 KSP residual norm ||r||_B = 9.635465e-06\n",
       "  9 KSP residual norm ||r||_B = 4.272494e-06\n",
       " 10 KSP residual norm ||r||_B = 2.145652e-06\n",
       " 11 KSP residual norm ||r||_B = 1.064721e-06\n",
       " 12 KSP residual norm ||r||_B = 8.968845e-07\n",
       " 13 KSP residual norm ||r||_B = 9.461616e-07\n",
       " 14 KSP residual norm ||r||_B = 4.844557e-07\n",
       " 15 KSP residual norm ||r||_B = 1.705841e-07\n",
       " 16 KSP residual norm ||r||_B = 5.222154e-08\n",
       " 17 KSP residual norm ||r||_B = 1.573809e-08\n",
       " 18 KSP residual norm ||r||_B = 3.971119e-09\n",
       " 19 KSP residual norm ||r||_B = 8.927523e-10\n",
       " 20 KSP residual norm ||r||_B = 1.881645e-10\n",
       " 21 KSP residual norm ||r||_B = 3.817386e-11\n",
       " 22 KSP residual norm ||r||_B = 8.038979e-12\n",
       " 23 KSP residual norm ||r||_B = 1.712088e-12\n",
       " 24 KSP residual norm ||r||_B = 3.796757e-13\n",
       " 25 KSP residual norm ||r||_B = 8.386432e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.552e-01)\n",
       " Sol. ||E|| = 1.560897e+01, ||B|| = 3.099665e-01\n",
       " Field energy E (2.960e-14 J) + H (6.103e-14 J) = 9.063e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 56/100: t = 2.800000e-01 ns (elapsed time = 2.46e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 5.522279e-06\n",
       "  1 KSP residual norm ||r||_B = 4.416085e-06\n",
       "  2 KSP residual norm ||r||_B = 5.561586e-06\n",
       "  3 KSP residual norm ||r||_B = 7.660028e-06\n",
       "  4 KSP residual norm ||r||_B = 1.160502e-05\n",
       "  5 KSP residual norm ||r||_B = 1.411488e-05\n",
       "  6 KSP residual norm ||r||_B = 1.463658e-05\n",
       "  7 KSP residual norm ||r||_B = 1.041798e-05\n",
       "  8 KSP residual norm ||r||_B = 5.872633e-06\n",
       "  9 KSP residual norm ||r||_B = 2.758103e-06\n",
       " 10 KSP residual norm ||r||_B = 1.413868e-06\n",
       " 11 KSP residual norm ||r||_B = 1.333186e-06\n",
       " 12 KSP residual norm ||r||_B = 1.289096e-06\n",
       " 13 KSP residual norm ||r||_B = 5.787391e-07\n",
       " 14 KSP residual norm ||r||_B = 2.037298e-07\n",
       " 15 KSP residual norm ||r||_B = 7.956385e-08\n",
       " 16 KSP residual norm ||r||_B = 2.067328e-08\n",
       " 17 KSP residual norm ||r||_B = 4.643932e-09\n",
       " 18 KSP residual norm ||r||_B = 1.094807e-09\n",
       " 19 KSP residual norm ||r||_B = 2.912698e-10\n",
       " 20 KSP residual norm ||r||_B = 7.383647e-11\n",
       " 21 KSP residual norm ||r||_B = 1.660269e-11\n",
       " 22 KSP residual norm ||r||_B = 3.522006e-12\n",
       " 23 KSP residual norm ||r||_B = 7.192773e-13\n",
       " 24 KSP residual norm ||r||_B = 1.595481e-13\n",
       "PCG solver converged in 24 iterations (avg. reduction factor: 4.543e-01)\n",
       " Sol. ||E|| = 1.469587e+01, ||B|| = 2.919847e-01\n",
       " Field energy E (2.623e-14 J) + H (5.416e-14 J) = 8.039e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 57\n",
       " Updating solution error estimates\n",
       "\n",
       "It 57/100: t = 2.850000e-01 ns (elapsed time = 2.51e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.189990e-05\n",
       "  1 KSP residual norm ||r||_B = 7.059248e-06\n",
       "  2 KSP residual norm ||r||_B = 5.612640e-06\n",
       "  3 KSP residual norm ||r||_B = 5.909709e-06\n",
       "  4 KSP residual norm ||r||_B = 6.593499e-06\n",
       "  5 KSP residual norm ||r||_B = 9.314853e-06\n",
       "  6 KSP residual norm ||r||_B = 1.512993e-05\n",
       "  7 KSP residual norm ||r||_B = 1.756608e-05\n",
       "  8 KSP residual norm ||r||_B = 1.064471e-05\n",
       "  9 KSP residual norm ||r||_B = 5.803496e-06\n",
       " 10 KSP residual norm ||r||_B = 4.949016e-06\n",
       " 11 KSP residual norm ||r||_B = 4.296633e-06\n",
       " 12 KSP residual norm ||r||_B = 3.524385e-06\n",
       " 13 KSP residual norm ||r||_B = 1.708445e-06\n",
       " 14 KSP residual norm ||r||_B = 5.679560e-07\n",
       " 15 KSP residual norm ||r||_B = 1.832055e-07\n",
       " 16 KSP residual norm ||r||_B = 5.583933e-08\n",
       " 17 KSP residual norm ||r||_B = 1.692270e-08\n",
       " 18 KSP residual norm ||r||_B = 4.369860e-09\n",
       " 19 KSP residual norm ||r||_B = 9.966265e-10\n",
       " 20 KSP residual norm ||r||_B = 2.079417e-10\n",
       " 21 KSP residual norm ||r||_B = 4.151346e-11\n",
       " 22 KSP residual norm ||r||_B = 8.764021e-12\n",
       " 23 KSP residual norm ||r||_B = 1.900990e-12\n",
       " 24 KSP residual norm ||r||_B = 4.188546e-13\n",
       " 25 KSP residual norm ||r||_B = 9.106603e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.667e-01)\n",
       " Sol. ||E|| = 1.350088e+01, ||B|| = 2.683744e-01\n",
       " Field energy E (2.214e-14 J) + H (4.575e-14 J) = 6.789e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 58/100: t = 2.900000e-01 ns (elapsed time = 2.55e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.272141e-06\n",
       "  1 KSP residual norm ||r||_B = 4.994742e-06\n",
       "  2 KSP residual norm ||r||_B = 5.913653e-06\n",
       "  3 KSP residual norm ||r||_B = 7.744440e-06\n",
       "  4 KSP residual norm ||r||_B = 1.152864e-05\n",
       "  5 KSP residual norm ||r||_B = 1.428156e-05\n",
       "  6 KSP residual norm ||r||_B = 1.607527e-05\n",
       "  7 KSP residual norm ||r||_B = 1.210610e-05\n",
       "  8 KSP residual norm ||r||_B = 7.449677e-06\n",
       "  9 KSP residual norm ||r||_B = 4.414196e-06\n",
       " 10 KSP residual norm ||r||_B = 3.406614e-06\n",
       " 11 KSP residual norm ||r||_B = 3.582902e-06\n",
       " 12 KSP residual norm ||r||_B = 2.045501e-06\n",
       " 13 KSP residual norm ||r||_B = 7.229910e-07\n",
       " 14 KSP residual norm ||r||_B = 2.511080e-07\n",
       " 15 KSP residual norm ||r||_B = 9.373662e-08\n",
       " 16 KSP residual norm ||r||_B = 2.340122e-08\n",
       " 17 KSP residual norm ||r||_B = 5.073640e-09\n",
       " 18 KSP residual norm ||r||_B = 1.119309e-09\n",
       " 19 KSP residual norm ||r||_B = 2.875379e-10\n",
       " 20 KSP residual norm ||r||_B = 7.595761e-11\n",
       " 21 KSP residual norm ||r||_B = 1.789851e-11\n",
       " 22 KSP residual norm ||r||_B = 3.846630e-12\n",
       " 23 KSP residual norm ||r||_B = 7.975760e-13\n",
       " 24 KSP residual norm ||r||_B = 1.786877e-13\n",
       " 25 KSP residual norm ||r||_B = 4.082809e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.563e-01)\n",
       " Sol. ||E|| = 1.211280e+01, ||B|| = 2.408976e-01\n",
       " Field energy E (1.782e-14 J) + H (3.686e-14 J) = 5.469e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 59\n",
       " Updating solution error estimates\n",
       "\n",
       "It 59/100: t = 2.950000e-01 ns (elapsed time = 2.59e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.152165e-05\n",
       "  1 KSP residual norm ||r||_B = 6.734203e-06\n",
       "  2 KSP residual norm ||r||_B = 5.343114e-06\n",
       "  3 KSP residual norm ||r||_B = 5.594810e-06\n",
       "  4 KSP residual norm ||r||_B = 6.161829e-06\n",
       "  5 KSP residual norm ||r||_B = 8.502533e-06\n",
       "  6 KSP residual norm ||r||_B = 1.350331e-05\n",
       "  7 KSP residual norm ||r||_B = 1.558456e-05\n",
       "  8 KSP residual norm ||r||_B = 1.014871e-05\n",
       "  9 KSP residual norm ||r||_B = 6.688483e-06\n",
       " 10 KSP residual norm ||r||_B = 6.788233e-06\n",
       " 11 KSP residual norm ||r||_B = 5.676300e-06\n",
       " 12 KSP residual norm ||r||_B = 3.911758e-06\n",
       " 13 KSP residual norm ||r||_B = 1.697157e-06\n",
       " 14 KSP residual norm ||r||_B = 5.497411e-07\n",
       " 15 KSP residual norm ||r||_B = 1.767901e-07\n",
       " 16 KSP residual norm ||r||_B = 5.388864e-08\n",
       " 17 KSP residual norm ||r||_B = 1.637784e-08\n",
       " 18 KSP residual norm ||r||_B = 4.250115e-09\n",
       " 19 KSP residual norm ||r||_B = 9.718973e-10\n",
       " 20 KSP residual norm ||r||_B = 2.028190e-10\n",
       " 21 KSP residual norm ||r||_B = 4.042868e-11\n",
       " 22 KSP residual norm ||r||_B = 8.533257e-12\n",
       " 23 KSP residual norm ||r||_B = 1.850993e-12\n",
       " 24 KSP residual norm ||r||_B = 4.078243e-13\n",
       " 25 KSP residual norm ||r||_B = 8.861614e-14\n",
       " 26 KSP residual norm ||r||_B = 1.928171e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.706e-01)\n",
       " Sol. ||E|| = 1.061784e+01, ||B|| = 2.112663e-01\n",
       " Field energy E (1.369e-14 J) + H (2.835e-14 J) = 4.205e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 60/100: t = 3.000000e-01 ns (elapsed time = 2.63e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.287456e-06\n",
       "  1 KSP residual norm ||r||_B = 4.205365e-06\n",
       "  2 KSP residual norm ||r||_B = 4.491241e-06\n",
       "  3 KSP residual norm ||r||_B = 5.950902e-06\n",
       "  4 KSP residual norm ||r||_B = 9.028222e-06\n",
       "  5 KSP residual norm ||r||_B = 1.145573e-05\n",
       "  6 KSP residual norm ||r||_B = 1.224134e-05\n",
       "  7 KSP residual norm ||r||_B = 1.066184e-05\n",
       "  8 KSP residual norm ||r||_B = 7.755818e-06\n",
       "  9 KSP residual norm ||r||_B = 4.735316e-06\n",
       " 10 KSP residual norm ||r||_B = 3.709539e-06\n",
       " 11 KSP residual norm ||r||_B = 3.824590e-06\n",
       " 12 KSP residual norm ||r||_B = 2.206733e-06\n",
       " 13 KSP residual norm ||r||_B = 6.959049e-07\n",
       " 14 KSP residual norm ||r||_B = 2.139906e-07\n",
       " 15 KSP residual norm ||r||_B = 8.648125e-08\n",
       " 16 KSP residual norm ||r||_B = 2.537799e-08\n",
       " 17 KSP residual norm ||r||_B = 6.511247e-09\n",
       " 18 KSP residual norm ||r||_B = 1.728867e-09\n",
       " 19 KSP residual norm ||r||_B = 4.437264e-10\n",
       " 20 KSP residual norm ||r||_B = 1.013216e-10\n",
       " 21 KSP residual norm ||r||_B = 2.164493e-11\n",
       " 22 KSP residual norm ||r||_B = 4.553265e-12\n",
       " 23 KSP residual norm ||r||_B = 9.189704e-13\n",
       " 24 KSP residual norm ||r||_B = 2.031399e-13\n",
       " 25 KSP residual norm ||r||_B = 4.660737e-14\n",
       " 26 KSP residual norm ||r||_B = 9.729938e-15\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.748e-01)\n",
       " Sol. ||E|| = 9.094385e+00, ||B|| = 1.810399e-01\n",
       " Field energy E (1.005e-14 J) + H (2.082e-14 J) = 3.087e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 61\n",
       " Updating solution error estimates\n",
       "\n",
       "It 61/100: t = 3.050000e-01 ns (elapsed time = 2.68e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.004687e-05\n",
       "  1 KSP residual norm ||r||_B = 5.428956e-06\n",
       "  2 KSP residual norm ||r||_B = 4.014531e-06\n",
       "  3 KSP residual norm ||r||_B = 4.018441e-06\n",
       "  4 KSP residual norm ||r||_B = 4.260151e-06\n",
       "  5 KSP residual norm ||r||_B = 5.527594e-06\n",
       "  6 KSP residual norm ||r||_B = 8.424912e-06\n",
       "  7 KSP residual norm ||r||_B = 1.044576e-05\n",
       "  8 KSP residual norm ||r||_B = 8.027515e-06\n",
       "  9 KSP residual norm ||r||_B = 5.917540e-06\n",
       " 10 KSP residual norm ||r||_B = 6.294079e-06\n",
       " 11 KSP residual norm ||r||_B = 5.408948e-06\n",
       " 12 KSP residual norm ||r||_B = 3.669658e-06\n",
       " 13 KSP residual norm ||r||_B = 1.523643e-06\n",
       " 14 KSP residual norm ||r||_B = 4.961740e-07\n",
       " 15 KSP residual norm ||r||_B = 1.609298e-07\n",
       " 16 KSP residual norm ||r||_B = 4.886299e-08\n",
       " 17 KSP residual norm ||r||_B = 1.483671e-08\n",
       " 18 KSP residual norm ||r||_B = 3.806052e-09\n",
       " 19 KSP residual norm ||r||_B = 8.625852e-10\n",
       " 20 KSP residual norm ||r||_B = 1.814362e-10\n",
       " 21 KSP residual norm ||r||_B = 3.657418e-11\n",
       " 22 KSP residual norm ||r||_B = 7.713746e-12\n",
       " 23 KSP residual norm ||r||_B = 1.647937e-12\n",
       " 24 KSP residual norm ||r||_B = 3.644642e-13\n",
       " 25 KSP residual norm ||r||_B = 8.016946e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.779e-01)\n",
       " Sol. ||E|| = 7.609217e+00, ||B|| = 1.515484e-01\n",
       " Field energy E (7.033e-15 J) + H (1.459e-14 J) = 2.162e-14 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 62/100: t = 3.100000e-01 ns (elapsed time = 2.72e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.368555e-06\n",
       "  1 KSP residual norm ||r||_B = 3.175730e-06\n",
       "  2 KSP residual norm ||r||_B = 2.465892e-06\n",
       "  3 KSP residual norm ||r||_B = 2.994258e-06\n",
       "  4 KSP residual norm ||r||_B = 4.901355e-06\n",
       "  5 KSP residual norm ||r||_B = 7.571743e-06\n",
       "  6 KSP residual norm ||r||_B = 7.447852e-06\n",
       "  7 KSP residual norm ||r||_B = 5.839455e-06\n",
       "  8 KSP residual norm ||r||_B = 5.555861e-06\n",
       "  9 KSP residual norm ||r||_B = 4.144054e-06\n",
       " 10 KSP residual norm ||r||_B = 2.694180e-06\n",
       " 11 KSP residual norm ||r||_B = 2.367078e-06\n",
       " 12 KSP residual norm ||r||_B = 1.977482e-06\n",
       " 13 KSP residual norm ||r||_B = 6.789335e-07\n",
       " 14 KSP residual norm ||r||_B = 1.587956e-07\n",
       " 15 KSP residual norm ||r||_B = 4.392392e-08\n",
       " 16 KSP residual norm ||r||_B = 1.094537e-08\n",
       " 17 KSP residual norm ||r||_B = 2.513422e-09\n",
       " 18 KSP residual norm ||r||_B = 6.823678e-10\n",
       " 19 KSP residual norm ||r||_B = 2.703931e-10\n",
       " 20 KSP residual norm ||r||_B = 9.464364e-11\n",
       " 21 KSP residual norm ||r||_B = 2.405371e-11\n",
       " 22 KSP residual norm ||r||_B = 5.243556e-12\n",
       " 23 KSP residual norm ||r||_B = 1.019130e-12\n",
       " 24 KSP residual norm ||r||_B = 2.221409e-13\n",
       " 25 KSP residual norm ||r||_B = 5.332957e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.738e-01)\n",
       " Sol. ||E|| = 6.215193e+00, ||B|| = 1.238466e-01\n",
       " Field energy E (4.692e-15 J) + H (9.743e-15 J) = 1.444e-14 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 63\n",
       " Updating solution error estimates\n",
       "\n",
       "It 63/100: t = 3.150000e-01 ns (elapsed time = 2.77e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.390420e-06\n",
       "  1 KSP residual norm ||r||_B = 3.950286e-06\n",
       "  2 KSP residual norm ||r||_B = 2.449177e-06\n",
       "  3 KSP residual norm ||r||_B = 2.121432e-06\n",
       "  4 KSP residual norm ||r||_B = 2.051082e-06\n",
       "  5 KSP residual norm ||r||_B = 2.323428e-06\n",
       "  6 KSP residual norm ||r||_B = 3.118875e-06\n",
       "  7 KSP residual norm ||r||_B = 4.155245e-06\n",
       "  8 KSP residual norm ||r||_B = 4.278766e-06\n",
       "  9 KSP residual norm ||r||_B = 3.536528e-06\n",
       " 10 KSP residual norm ||r||_B = 3.868730e-06\n",
       " 11 KSP residual norm ||r||_B = 3.930835e-06\n",
       " 12 KSP residual norm ||r||_B = 3.072276e-06\n",
       " 13 KSP residual norm ||r||_B = 1.281272e-06\n",
       " 14 KSP residual norm ||r||_B = 4.289561e-07\n",
       " 15 KSP residual norm ||r||_B = 1.423209e-07\n",
       " 16 KSP residual norm ||r||_B = 4.292158e-08\n",
       " 17 KSP residual norm ||r||_B = 1.305309e-08\n",
       " 18 KSP residual norm ||r||_B = 3.285872e-09\n",
       " 19 KSP residual norm ||r||_B = 7.305594e-10\n",
       " 20 KSP residual norm ||r||_B = 1.559127e-10\n",
       " 21 KSP residual norm ||r||_B = 3.224020e-11\n",
       " 22 KSP residual norm ||r||_B = 6.787408e-12\n",
       " 23 KSP residual norm ||r||_B = 1.403229e-12\n",
       " 24 KSP residual norm ||r||_B = 3.118144e-13\n",
       " 25 KSP residual norm ||r||_B = 7.066539e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.667e-01)\n",
       " Sol. ||E|| = 4.950382e+00, ||B|| = 9.869571e-02\n",
       " Field energy E (2.977e-15 J) + H (6.188e-15 J) = 9.165e-15 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 64/100: t = 3.200000e-01 ns (elapsed time = 2.80e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.994151e-06\n",
       "  1 KSP residual norm ||r||_B = 2.878016e-06\n",
       "  2 KSP residual norm ||r||_B = 1.376720e-06\n",
       "  3 KSP residual norm ||r||_B = 8.969037e-07\n",
       "  4 KSP residual norm ||r||_B = 9.590531e-07\n",
       "  5 KSP residual norm ||r||_B = 1.687905e-06\n",
       "  6 KSP residual norm ||r||_B = 3.079305e-06\n",
       "  7 KSP residual norm ||r||_B = 2.815180e-06\n",
       "  8 KSP residual norm ||r||_B = 2.026876e-06\n",
       "  9 KSP residual norm ||r||_B = 1.754117e-06\n",
       " 10 KSP residual norm ||r||_B = 1.467859e-06\n",
       " 11 KSP residual norm ||r||_B = 8.341040e-07\n",
       " 12 KSP residual norm ||r||_B = 7.160125e-07\n",
       " 13 KSP residual norm ||r||_B = 6.117894e-07\n",
       " 14 KSP residual norm ||r||_B = 2.556452e-07\n",
       " 15 KSP residual norm ||r||_B = 9.961670e-08\n",
       " 16 KSP residual norm ||r||_B = 3.223495e-08\n",
       " 17 KSP residual norm ||r||_B = 1.048012e-08\n",
       " 18 KSP residual norm ||r||_B = 2.737544e-09\n",
       " 19 KSP residual norm ||r||_B = 5.964253e-10\n",
       " 20 KSP residual norm ||r||_B = 1.294705e-10\n",
       " 21 KSP residual norm ||r||_B = 2.839004e-11\n",
       " 22 KSP residual norm ||r||_B = 5.968317e-12\n",
       " 23 KSP residual norm ||r||_B = 1.137945e-12\n",
       " 24 KSP residual norm ||r||_B = 2.489244e-13\n",
       " 25 KSP residual norm ||r||_B = 6.136017e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.684e-01)\n",
       " Sol. ||E|| = 3.838435e+00, ||B|| = 7.657056e-02\n",
       " Field energy E (1.790e-15 J) + H (3.724e-15 J) = 5.514e-15 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 65\n",
       " Updating solution error estimates\n",
       "\n",
       "It 65/100: t = 3.250000e-01 ns (elapsed time = 2.85e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.294289e-06\n",
       "  1 KSP residual norm ||r||_B = 3.007638e-06\n",
       "  2 KSP residual norm ||r||_B = 1.453619e-06\n",
       "  3 KSP residual norm ||r||_B = 8.883695e-07\n",
       "  4 KSP residual norm ||r||_B = 6.335122e-07\n",
       "  5 KSP residual norm ||r||_B = 5.058135e-07\n",
       "  6 KSP residual norm ||r||_B = 4.052048e-07\n",
       "  7 KSP residual norm ||r||_B = 3.326861e-07\n",
       "  8 KSP residual norm ||r||_B = 3.434537e-07\n",
       "  9 KSP residual norm ||r||_B = 3.145019e-07\n",
       " 10 KSP residual norm ||r||_B = 3.287960e-07\n",
       " 11 KSP residual norm ||r||_B = 4.362757e-07\n",
       " 12 KSP residual norm ||r||_B = 8.181378e-07\n",
       " 13 KSP residual norm ||r||_B = 8.230233e-07\n",
       " 14 KSP residual norm ||r||_B = 3.453106e-07\n",
       " 15 KSP residual norm ||r||_B = 1.237147e-07\n",
       " 16 KSP residual norm ||r||_B = 3.758496e-08\n",
       " 17 KSP residual norm ||r||_B = 1.160128e-08\n",
       " 18 KSP residual norm ||r||_B = 2.908634e-09\n",
       " 19 KSP residual norm ||r||_B = 6.335785e-10\n",
       " 20 KSP residual norm ||r||_B = 1.368496e-10\n",
       " 21 KSP residual norm ||r||_B = 2.925437e-11\n",
       " 22 KSP residual norm ||r||_B = 6.154014e-12\n",
       " 23 KSP residual norm ||r||_B = 1.216197e-12\n",
       " 24 KSP residual norm ||r||_B = 2.689272e-13\n",
       " 25 KSP residual norm ||r||_B = 6.382211e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.629e-01)\n",
       " Sol. ||E|| = 2.890002e+00, ||B|| = 5.768734e-02\n",
       " Field energy E (1.015e-15 J) + H (2.114e-15 J) = 3.129e-15 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 66/100: t = 3.300000e-01 ns (elapsed time = 2.89e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.811757e-06\n",
       "  1 KSP residual norm ||r||_B = 3.190473e-06\n",
       "  2 KSP residual norm ||r||_B = 1.434268e-06\n",
       "  3 KSP residual norm ||r||_B = 7.516964e-07\n",
       "  4 KSP residual norm ||r||_B = 4.496482e-07\n",
       "  5 KSP residual norm ||r||_B = 3.471965e-07\n",
       "  6 KSP residual norm ||r||_B = 3.333867e-07\n",
       "  7 KSP residual norm ||r||_B = 3.563672e-07\n",
       "  8 KSP residual norm ||r||_B = 5.403417e-07\n",
       "  9 KSP residual norm ||r||_B = 7.854647e-07\n",
       " 10 KSP residual norm ||r||_B = 7.655687e-07\n",
       " 11 KSP residual norm ||r||_B = 5.312321e-07\n",
       " 12 KSP residual norm ||r||_B = 6.152642e-07\n",
       " 13 KSP residual norm ||r||_B = 6.955750e-07\n",
       " 14 KSP residual norm ||r||_B = 3.417506e-07\n",
       " 15 KSP residual norm ||r||_B = 1.294196e-07\n",
       " 16 KSP residual norm ||r||_B = 3.990021e-08\n",
       " 17 KSP residual norm ||r||_B = 1.241395e-08\n",
       " 18 KSP residual norm ||r||_B = 3.107848e-09\n",
       " 19 KSP residual norm ||r||_B = 6.734482e-10\n",
       " 20 KSP residual norm ||r||_B = 1.459965e-10\n",
       " 21 KSP residual norm ||r||_B = 3.153732e-11\n",
       " 22 KSP residual norm ||r||_B = 6.614123e-12\n",
       " 23 KSP residual norm ||r||_B = 1.289219e-12\n",
       " 24 KSP residual norm ||r||_B = 2.852636e-13\n",
       " 25 KSP residual norm ||r||_B = 6.879200e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.702e-01)\n",
       " Sol. ||E|| = 2.104792e+00, ||B|| = 4.204435e-02\n",
       " Field energy E (5.382e-16 J) + H (1.123e-15 J) = 1.661e-15 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 67\n",
       " Updating solution error estimates\n",
       "\n",
       "It 67/100: t = 3.350000e-01 ns (elapsed time = 2.94e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 6.928115e-06\n",
       "  1 KSP residual norm ||r||_B = 2.755058e-06\n",
       "  2 KSP residual norm ||r||_B = 1.289447e-06\n",
       "  3 KSP residual norm ||r||_B = 7.972152e-07\n",
       "  4 KSP residual norm ||r||_B = 7.505405e-07\n",
       "  5 KSP residual norm ||r||_B = 1.064461e-06\n",
       "  6 KSP residual norm ||r||_B = 1.419480e-06\n",
       "  7 KSP residual norm ||r||_B = 1.234279e-06\n",
       "  8 KSP residual norm ||r||_B = 1.372613e-06\n",
       "  9 KSP residual norm ||r||_B = 1.839607e-06\n",
       " 10 KSP residual norm ||r||_B = 1.924927e-06\n",
       " 11 KSP residual norm ||r||_B = 1.391399e-06\n",
       " 12 KSP residual norm ||r||_B = 1.281298e-06\n",
       " 13 KSP residual norm ||r||_B = 7.794750e-07\n",
       " 14 KSP residual norm ||r||_B = 2.834187e-07\n",
       " 15 KSP residual norm ||r||_B = 1.059475e-07\n",
       " 16 KSP residual norm ||r||_B = 3.338958e-08\n",
       " 17 KSP residual norm ||r||_B = 1.067241e-08\n",
       " 18 KSP residual norm ||r||_B = 2.751832e-09\n",
       " 19 KSP residual norm ||r||_B = 5.971610e-10\n",
       " 20 KSP residual norm ||r||_B = 1.292430e-10\n",
       " 21 KSP residual norm ||r||_B = 2.821439e-11\n",
       " 22 KSP residual norm ||r||_B = 5.956116e-12\n",
       " 23 KSP residual norm ||r||_B = 1.142245e-12\n",
       " 24 KSP residual norm ||r||_B = 2.488505e-13\n",
       " 25 KSP residual norm ||r||_B = 6.098200e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.638e-01)\n",
       " Sol. ||E|| = 1.474050e+00, ||B|| = 2.947075e-02\n",
       " Field energy E (2.639e-16 J) + H (5.517e-16 J) = 8.157e-16 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 68/100: t = 3.400000e-01 ns (elapsed time = 2.97e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.380265e-06\n",
       "  1 KSP residual norm ||r||_B = 3.509493e-06\n",
       "  2 KSP residual norm ||r||_B = 1.746477e-06\n",
       "  3 KSP residual norm ||r||_B = 1.190352e-06\n",
       "  4 KSP residual norm ||r||_B = 1.067864e-06\n",
       "  5 KSP residual norm ||r||_B = 1.227643e-06\n",
       "  6 KSP residual norm ||r||_B = 1.556039e-06\n",
       "  7 KSP residual norm ||r||_B = 2.004482e-06\n",
       "  8 KSP residual norm ||r||_B = 2.711362e-06\n",
       "  9 KSP residual norm ||r||_B = 2.413547e-06\n",
       " 10 KSP residual norm ||r||_B = 1.933388e-06\n",
       " 11 KSP residual norm ||r||_B = 1.764822e-06\n",
       " 12 KSP residual norm ||r||_B = 1.990954e-06\n",
       " 13 KSP residual norm ||r||_B = 1.129227e-06\n",
       " 14 KSP residual norm ||r||_B = 4.097488e-07\n",
       " 15 KSP residual norm ||r||_B = 1.430019e-07\n",
       " 16 KSP residual norm ||r||_B = 4.339985e-08\n",
       " 17 KSP residual norm ||r||_B = 1.338453e-08\n",
       " 18 KSP residual norm ||r||_B = 3.340516e-09\n",
       " 19 KSP residual norm ||r||_B = 7.280051e-10\n",
       " 20 KSP residual norm ||r||_B = 1.572911e-10\n",
       " 21 KSP residual norm ||r||_B = 3.358073e-11\n",
       " 22 KSP residual norm ||r||_B = 7.051339e-12\n",
       " 23 KSP residual norm ||r||_B = 1.398140e-12\n",
       " 24 KSP residual norm ||r||_B = 3.102800e-13\n",
       " 25 KSP residual norm ||r||_B = 7.345866e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.751e-01)\n",
       " Sol. ||E|| = 9.830679e-01, ||B|| = 1.967675e-02\n",
       " Field energy E (1.174e-16 J) + H (2.460e-16 J) = 3.634e-16 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 69\n",
       " Updating solution error estimates\n",
       "\n",
       "It 69/100: t = 3.450000e-01 ns (elapsed time = 3.02e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.011577e-06\n",
       "  1 KSP residual norm ||r||_B = 2.815072e-06\n",
       "  2 KSP residual norm ||r||_B = 1.412524e-06\n",
       "  3 KSP residual norm ||r||_B = 1.030517e-06\n",
       "  4 KSP residual norm ||r||_B = 1.249329e-06\n",
       "  5 KSP residual norm ||r||_B = 2.266264e-06\n",
       "  6 KSP residual norm ||r||_B = 3.605388e-06\n",
       "  7 KSP residual norm ||r||_B = 2.666045e-06\n",
       "  8 KSP residual norm ||r||_B = 2.012231e-06\n",
       "  9 KSP residual norm ||r||_B = 2.343614e-06\n",
       " 10 KSP residual norm ||r||_B = 2.456588e-06\n",
       " 11 KSP residual norm ||r||_B = 1.030829e-06\n",
       " 12 KSP residual norm ||r||_B = 4.031174e-07\n",
       " 13 KSP residual norm ||r||_B = 2.679567e-07\n",
       " 14 KSP residual norm ||r||_B = 1.630174e-07\n",
       " 15 KSP residual norm ||r||_B = 8.289674e-08\n",
       " 16 KSP residual norm ||r||_B = 3.001210e-08\n",
       " 17 KSP residual norm ||r||_B = 1.019966e-08\n",
       " 18 KSP residual norm ||r||_B = 2.745543e-09\n",
       " 19 KSP residual norm ||r||_B = 6.016871e-10\n",
       " 20 KSP residual norm ||r||_B = 1.301489e-10\n",
       " 21 KSP residual norm ||r||_B = 2.857187e-11\n",
       " 22 KSP residual norm ||r||_B = 6.053320e-12\n",
       " 23 KSP residual norm ||r||_B = 1.152556e-12\n",
       " 24 KSP residual norm ||r||_B = 2.492446e-13\n",
       " 25 KSP residual norm ||r||_B = 6.151039e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.680e-01)\n",
       " Sol. ||E|| = 6.135914e-01, ||B|| = 1.230114e-02\n",
       " Field energy E (4.574e-17 J) + H (9.613e-17 J) = 1.419e-16 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 70/100: t = 3.500000e-01 ns (elapsed time = 3.06e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.596533e-06\n",
       "  1 KSP residual norm ||r||_B = 3.593978e-06\n",
       "  2 KSP residual norm ||r||_B = 1.838806e-06\n",
       "  3 KSP residual norm ||r||_B = 1.341306e-06\n",
       "  4 KSP residual norm ||r||_B = 1.299568e-06\n",
       "  5 KSP residual norm ||r||_B = 1.542596e-06\n",
       "  6 KSP residual norm ||r||_B = 1.914581e-06\n",
       "  7 KSP residual norm ||r||_B = 2.350843e-06\n",
       "  8 KSP residual norm ||r||_B = 2.987202e-06\n",
       "  9 KSP residual norm ||r||_B = 2.647714e-06\n",
       " 10 KSP residual norm ||r||_B = 2.359794e-06\n",
       " 11 KSP residual norm ||r||_B = 2.341441e-06\n",
       " 12 KSP residual norm ||r||_B = 2.418520e-06\n",
       " 13 KSP residual norm ||r||_B = 1.204889e-06\n",
       " 14 KSP residual norm ||r||_B = 4.231461e-07\n",
       " 15 KSP residual norm ||r||_B = 1.466052e-07\n",
       " 16 KSP residual norm ||r||_B = 4.446474e-08\n",
       " 17 KSP residual norm ||r||_B = 1.372454e-08\n",
       " 18 KSP residual norm ||r||_B = 3.434778e-09\n",
       " 19 KSP residual norm ||r||_B = 7.501683e-10\n",
       " 20 KSP residual norm ||r||_B = 1.618496e-10\n",
       " 21 KSP residual norm ||r||_B = 3.445598e-11\n",
       " 22 KSP residual norm ||r||_B = 7.245132e-12\n",
       " 23 KSP residual norm ||r||_B = 1.442386e-12\n",
       " 24 KSP residual norm ||r||_B = 3.198465e-13\n",
       " 25 KSP residual norm ||r||_B = 7.540505e-14\n",
       " 26 KSP residual norm ||r||_B = 1.589988e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.667e-01)\n",
       " Sol. ||E|| = 3.458650e-01, ||B|| = 6.952284e-03\n",
       " Field energy E (1.453e-17 J) + H (3.071e-17 J) = 4.524e-17 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 71\n",
       " Updating solution error estimates\n",
       "\n",
       "It 71/100: t = 3.550000e-01 ns (elapsed time = 3.11e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.274001e-06\n",
       "  1 KSP residual norm ||r||_B = 2.901289e-06\n",
       "  2 KSP residual norm ||r||_B = 1.436935e-06\n",
       "  3 KSP residual norm ||r||_B = 1.013097e-06\n",
       "  4 KSP residual norm ||r||_B = 1.182401e-06\n",
       "  5 KSP residual norm ||r||_B = 2.132627e-06\n",
       "  6 KSP residual norm ||r||_B = 3.601632e-06\n",
       "  7 KSP residual norm ||r||_B = 2.848365e-06\n",
       "  8 KSP residual norm ||r||_B = 2.059781e-06\n",
       "  9 KSP residual norm ||r||_B = 2.120440e-06\n",
       " 10 KSP residual norm ||r||_B = 2.077136e-06\n",
       " 11 KSP residual norm ||r||_B = 1.103359e-06\n",
       " 12 KSP residual norm ||r||_B = 7.680862e-07\n",
       " 13 KSP residual norm ||r||_B = 5.997524e-07\n",
       " 14 KSP residual norm ||r||_B = 2.410624e-07\n",
       " 15 KSP residual norm ||r||_B = 9.328332e-08\n",
       " 16 KSP residual norm ||r||_B = 3.099780e-08\n",
       " 17 KSP residual norm ||r||_B = 1.046572e-08\n",
       " 18 KSP residual norm ||r||_B = 2.841065e-09\n",
       " 19 KSP residual norm ||r||_B = 6.245094e-10\n",
       " 20 KSP residual norm ||r||_B = 1.350532e-10\n",
       " 21 KSP residual norm ||r||_B = 2.966440e-11\n",
       " 22 KSP residual norm ||r||_B = 6.292670e-12\n",
       " 23 KSP residual norm ||r||_B = 1.198220e-12\n",
       " 24 KSP residual norm ||r||_B = 2.588899e-13\n",
       " 25 KSP residual norm ||r||_B = 6.391296e-14\n",
       "PCG solver converged in 25 iterations (avg. reduction factor: 4.743e-01)\n",
       " Sol. ||E|| = 1.603032e-01, ||B|| = 3.241204e-03\n",
       " Field energy E (3.122e-18 J) + H (6.674e-18 J) = 9.796e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 72/100: t = 3.600000e-01 ns (elapsed time = 3.15e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.585511e-06\n",
       "  1 KSP residual norm ||r||_B = 3.503105e-06\n",
       "  2 KSP residual norm ||r||_B = 1.732795e-06\n",
       "  3 KSP residual norm ||r||_B = 1.208105e-06\n",
       "  4 KSP residual norm ||r||_B = 1.143529e-06\n",
       "  5 KSP residual norm ||r||_B = 1.339476e-06\n",
       "  6 KSP residual norm ||r||_B = 1.575745e-06\n",
       "  7 KSP residual norm ||r||_B = 1.775739e-06\n",
       "  8 KSP residual norm ||r||_B = 2.276599e-06\n",
       "  9 KSP residual norm ||r||_B = 2.246829e-06\n",
       " 10 KSP residual norm ||r||_B = 2.177658e-06\n",
       " 11 KSP residual norm ||r||_B = 2.236506e-06\n",
       " 12 KSP residual norm ||r||_B = 2.351815e-06\n",
       " 13 KSP residual norm ||r||_B = 1.185136e-06\n",
       " 14 KSP residual norm ||r||_B = 4.155300e-07\n",
       " 15 KSP residual norm ||r||_B = 1.452077e-07\n",
       " 16 KSP residual norm ||r||_B = 4.417059e-08\n",
       " 17 KSP residual norm ||r||_B = 1.370297e-08\n",
       " 18 KSP residual norm ||r||_B = 3.442505e-09\n",
       " 19 KSP residual norm ||r||_B = 7.508815e-10\n",
       " 20 KSP residual norm ||r||_B = 1.620563e-10\n",
       " 21 KSP residual norm ||r||_B = 3.462148e-11\n",
       " 22 KSP residual norm ||r||_B = 7.289809e-12\n",
       " 23 KSP residual norm ||r||_B = 1.444408e-12\n",
       " 24 KSP residual norm ||r||_B = 3.194883e-13\n",
       " 25 KSP residual norm ||r||_B = 7.572077e-14\n",
       " 26 KSP residual norm ||r||_B = 1.597288e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.730e-01)\n",
       " Sol. ||E|| = 3.869602e-02, ||B|| = 8.055977e-04\n",
       " Field energy E (1.819e-19 J) + H (4.124e-19 J) = 5.943e-19 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 73\n",
       " Updating solution error estimates\n",
       "\n",
       "It 73/100: t = 3.650000e-01 ns (elapsed time = 3.20e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.594508e-06\n",
       "  1 KSP residual norm ||r||_B = 2.971055e-06\n",
       "  2 KSP residual norm ||r||_B = 1.384905e-06\n",
       "  3 KSP residual norm ||r||_B = 8.484744e-07\n",
       "  4 KSP residual norm ||r||_B = 8.267039e-07\n",
       "  5 KSP residual norm ||r||_B = 1.351565e-06\n",
       "  6 KSP residual norm ||r||_B = 2.394100e-06\n",
       "  7 KSP residual norm ||r||_B = 2.132597e-06\n",
       "  8 KSP residual norm ||r||_B = 1.655062e-06\n",
       "  9 KSP residual norm ||r||_B = 1.875703e-06\n",
       " 10 KSP residual norm ||r||_B = 2.134395e-06\n",
       " 11 KSP residual norm ||r||_B = 1.131362e-06\n",
       " 12 KSP residual norm ||r||_B = 6.780246e-07\n",
       " 13 KSP residual norm ||r||_B = 5.393423e-07\n",
       " 14 KSP residual norm ||r||_B = 2.466265e-07\n",
       " 15 KSP residual norm ||r||_B = 1.000387e-07\n",
       " 16 KSP residual norm ||r||_B = 3.334146e-08\n",
       " 17 KSP residual norm ||r||_B = 1.115580e-08\n",
       " 18 KSP residual norm ||r||_B = 2.989902e-09\n",
       " 19 KSP residual norm ||r||_B = 6.544691e-10\n",
       " 20 KSP residual norm ||r||_B = 1.414783e-10\n",
       " 21 KSP residual norm ||r||_B = 3.104706e-11\n",
       " 22 KSP residual norm ||r||_B = 6.585830e-12\n",
       " 23 KSP residual norm ||r||_B = 1.256378e-12\n",
       " 24 KSP residual norm ||r||_B = 2.718467e-13\n",
       " 25 KSP residual norm ||r||_B = 6.706066e-14\n",
       " 26 KSP residual norm ||r||_B = 1.419120e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.660e-01)\n",
       " Sol. ||E|| = 3.517864e-02, ||B|| = 6.753277e-04\n",
       " Field energy E (1.503e-19 J) + H (2.896e-19 J) = 4.399e-19 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 74/100: t = 3.700000e-01 ns (elapsed time = 3.25e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.512817e-06\n",
       "  1 KSP residual norm ||r||_B = 3.367686e-06\n",
       "  2 KSP residual norm ||r||_B = 1.570884e-06\n",
       "  3 KSP residual norm ||r||_B = 9.820963e-07\n",
       "  4 KSP residual norm ||r||_B = 8.446378e-07\n",
       "  5 KSP residual norm ||r||_B = 9.500773e-07\n",
       "  6 KSP residual norm ||r||_B = 1.049631e-06\n",
       "  7 KSP residual norm ||r||_B = 1.023560e-06\n",
       "  8 KSP residual norm ||r||_B = 1.286661e-06\n",
       "  9 KSP residual norm ||r||_B = 1.493649e-06\n",
       " 10 KSP residual norm ||r||_B = 1.605335e-06\n",
       " 11 KSP residual norm ||r||_B = 1.673581e-06\n",
       " 12 KSP residual norm ||r||_B = 1.937389e-06\n",
       " 13 KSP residual norm ||r||_B = 1.108570e-06\n",
       " 14 KSP residual norm ||r||_B = 3.973246e-07\n",
       " 15 KSP residual norm ||r||_B = 1.414434e-07\n",
       " 16 KSP residual norm ||r||_B = 4.331617e-08\n",
       " 17 KSP residual norm ||r||_B = 1.354765e-08\n",
       " 18 KSP residual norm ||r||_B = 3.423101e-09\n",
       " 19 KSP residual norm ||r||_B = 7.448886e-10\n",
       " 20 KSP residual norm ||r||_B = 1.608663e-10\n",
       " 21 KSP residual norm ||r||_B = 3.458087e-11\n",
       " 22 KSP residual norm ||r||_B = 7.293666e-12\n",
       " 23 KSP residual norm ||r||_B = 1.433158e-12\n",
       " 24 KSP residual norm ||r||_B = 3.157439e-13\n",
       " 25 KSP residual norm ||r||_B = 7.553773e-14\n",
       " 26 KSP residual norm ||r||_B = 1.593903e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.758e-01)\n",
       " Sol. ||E|| = 7.467623e-02, ||B|| = 1.470800e-03\n",
       " Field energy E (6.774e-19 J) + H (1.374e-18 J) = 2.051e-18 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 75\n",
       " Updating solution error estimates\n",
       "\n",
       "It 75/100: t = 3.750000e-01 ns (elapsed time = 3.30e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 7.918968e-06\n",
       "  1 KSP residual norm ||r||_B = 3.043468e-06\n",
       "  2 KSP residual norm ||r||_B = 1.344875e-06\n",
       "  3 KSP residual norm ||r||_B = 7.112176e-07\n",
       "  4 KSP residual norm ||r||_B = 5.323337e-07\n",
       "  5 KSP residual norm ||r||_B = 6.924233e-07\n",
       "  6 KSP residual norm ||r||_B = 1.137911e-06\n",
       "  7 KSP residual norm ||r||_B = 1.055559e-06\n",
       "  8 KSP residual norm ||r||_B = 9.082845e-07\n",
       "  9 KSP residual norm ||r||_B = 1.235485e-06\n",
       " 10 KSP residual norm ||r||_B = 1.925303e-06\n",
       " 11 KSP residual norm ||r||_B = 1.115930e-06\n",
       " 12 KSP residual norm ||r||_B = 4.558241e-07\n",
       " 13 KSP residual norm ||r||_B = 2.936578e-07\n",
       " 14 KSP residual norm ||r||_B = 1.824423e-07\n",
       " 15 KSP residual norm ||r||_B = 9.689354e-08\n",
       " 16 KSP residual norm ||r||_B = 3.523559e-08\n",
       " 17 KSP residual norm ||r||_B = 1.186076e-08\n",
       " 18 KSP residual norm ||r||_B = 3.142935e-09\n",
       " 19 KSP residual norm ||r||_B = 6.854149e-10\n",
       " 20 KSP residual norm ||r||_B = 1.481129e-10\n",
       " 21 KSP residual norm ||r||_B = 3.244325e-11\n",
       " 22 KSP residual norm ||r||_B = 6.880771e-12\n",
       " 23 KSP residual norm ||r||_B = 1.316828e-12\n",
       " 24 KSP residual norm ||r||_B = 2.855135e-13\n",
       " 25 KSP residual norm ||r||_B = 7.027263e-14\n",
       " 26 KSP residual norm ||r||_B = 1.486896e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.708e-01)\n",
       " Sol. ||E|| = 9.085995e-02, ||B|| = 1.799539e-03\n",
       " Field energy E (1.003e-18 J) + H (2.057e-18 J) = 3.060e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 76/100: t = 3.800000e-01 ns (elapsed time = 3.34e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.482024e-06\n",
       "  1 KSP residual norm ||r||_B = 3.270570e-06\n",
       "  2 KSP residual norm ||r||_B = 1.450935e-06\n",
       "  3 KSP residual norm ||r||_B = 8.048359e-07\n",
       "  4 KSP residual norm ||r||_B = 5.964386e-07\n",
       "  5 KSP residual norm ||r||_B = 6.162260e-07\n",
       "  6 KSP residual norm ||r||_B = 6.402187e-07\n",
       "  7 KSP residual norm ||r||_B = 5.037948e-07\n",
       "  8 KSP residual norm ||r||_B = 5.433935e-07\n",
       "  9 KSP residual norm ||r||_B = 7.277138e-07\n",
       " 10 KSP residual norm ||r||_B = 9.460765e-07\n",
       " 11 KSP residual norm ||r||_B = 9.825481e-07\n",
       " 12 KSP residual norm ||r||_B = 1.240906e-06\n",
       " 13 KSP residual norm ||r||_B = 9.564955e-07\n",
       " 14 KSP residual norm ||r||_B = 3.727148e-07\n",
       " 15 KSP residual norm ||r||_B = 1.369084e-07\n",
       " 16 KSP residual norm ||r||_B = 4.241675e-08\n",
       " 17 KSP residual norm ||r||_B = 1.340439e-08\n",
       " 18 KSP residual norm ||r||_B = 3.414462e-09\n",
       " 19 KSP residual norm ||r||_B = 7.419214e-10\n",
       " 20 KSP residual norm ||r||_B = 1.602483e-10\n",
       " 21 KSP residual norm ||r||_B = 3.465196e-11\n",
       " 22 KSP residual norm ||r||_B = 7.323916e-12\n",
       " 23 KSP residual norm ||r||_B = 1.427886e-12\n",
       " 24 KSP residual norm ||r||_B = 3.131284e-13\n",
       " 25 KSP residual norm ||r||_B = 7.558737e-14\n",
       " 26 KSP residual norm ||r||_B = 1.596573e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.753e-01)\n",
       " Sol. ||E|| = 9.217384e-02, ||B|| = 1.830261e-03\n",
       " Field energy E (1.032e-18 J) + H (2.128e-18 J) = 3.160e-18 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 77\n",
       " Updating solution error estimates\n",
       "\n",
       "It 77/100: t = 3.850000e-01 ns (elapsed time = 3.39e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.213498e-06\n",
       "  1 KSP residual norm ||r||_B = 3.117339e-06\n",
       "  2 KSP residual norm ||r||_B = 1.340910e-06\n",
       "  3 KSP residual norm ||r||_B = 6.555524e-07\n",
       "  4 KSP residual norm ||r||_B = 3.977846e-07\n",
       "  5 KSP residual norm ||r||_B = 3.881862e-07\n",
       "  6 KSP residual norm ||r||_B = 5.064734e-07\n",
       "  7 KSP residual norm ||r||_B = 4.057976e-07\n",
       "  8 KSP residual norm ||r||_B = 3.299569e-07\n",
       "  9 KSP residual norm ||r||_B = 4.672426e-07\n",
       " 10 KSP residual norm ||r||_B = 1.011777e-06\n",
       " 11 KSP residual norm ||r||_B = 9.941826e-07\n",
       " 12 KSP residual norm ||r||_B = 3.760622e-07\n",
       " 13 KSP residual norm ||r||_B = 1.532265e-07\n",
       " 14 KSP residual norm ||r||_B = 6.241985e-08\n",
       " 15 KSP residual norm ||r||_B = 3.852528e-08\n",
       " 16 KSP residual norm ||r||_B = 2.535548e-08\n",
       " 17 KSP residual norm ||r||_B = 1.152576e-08\n",
       " 18 KSP residual norm ||r||_B = 3.252595e-09\n",
       " 19 KSP residual norm ||r||_B = 7.133309e-10\n",
       " 20 KSP residual norm ||r||_B = 1.541514e-10\n",
       " 21 KSP residual norm ||r||_B = 3.369936e-11\n",
       " 22 KSP residual norm ||r||_B = 7.148640e-12\n",
       " 23 KSP residual norm ||r||_B = 1.372900e-12\n",
       " 24 KSP residual norm ||r||_B = 2.981419e-13\n",
       " 25 KSP residual norm ||r||_B = 7.316529e-14\n",
       " 26 KSP residual norm ||r||_B = 1.548727e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.733e-01)\n",
       " Sol. ||E|| = 8.486363e-02, ||B|| = 1.687731e-03\n",
       " Field energy E (8.748e-19 J) + H (1.809e-18 J) = 2.684e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 78/100: t = 3.900000e-01 ns (elapsed time = 3.43e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.523205e-06\n",
       "  1 KSP residual norm ||r||_B = 3.229372e-06\n",
       "  2 KSP residual norm ||r||_B = 1.393554e-06\n",
       "  3 KSP residual norm ||r||_B = 7.134967e-07\n",
       "  4 KSP residual norm ||r||_B = 4.623899e-07\n",
       "  5 KSP residual norm ||r||_B = 4.296140e-07\n",
       "  6 KSP residual norm ||r||_B = 4.240098e-07\n",
       "  7 KSP residual norm ||r||_B = 2.620227e-07\n",
       "  8 KSP residual norm ||r||_B = 1.949587e-07\n",
       "  9 KSP residual norm ||r||_B = 2.394923e-07\n",
       " 10 KSP residual norm ||r||_B = 4.135748e-07\n",
       " 11 KSP residual norm ||r||_B = 4.790810e-07\n",
       " 12 KSP residual norm ||r||_B = 5.458128e-07\n",
       " 13 KSP residual norm ||r||_B = 6.303365e-07\n",
       " 14 KSP residual norm ||r||_B = 3.285936e-07\n",
       " 15 KSP residual norm ||r||_B = 1.314905e-07\n",
       " 16 KSP residual norm ||r||_B = 4.170066e-08\n",
       " 17 KSP residual norm ||r||_B = 1.333979e-08\n",
       " 18 KSP residual norm ||r||_B = 3.430031e-09\n",
       " 19 KSP residual norm ||r||_B = 7.452789e-10\n",
       " 20 KSP residual norm ||r||_B = 1.609166e-10\n",
       " 21 KSP residual norm ||r||_B = 3.494382e-11\n",
       " 22 KSP residual norm ||r||_B = 7.401710e-12\n",
       " 23 KSP residual norm ||r||_B = 1.435365e-12\n",
       " 24 KSP residual norm ||r||_B = 3.134587e-13\n",
       " 25 KSP residual norm ||r||_B = 7.614903e-14\n",
       " 26 KSP residual norm ||r||_B = 1.610972e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.745e-01)\n",
       " Sol. ||E|| = 7.331862e-02, ||B|| = 1.459731e-03\n",
       " Field energy E (6.530e-19 J) + H (1.354e-18 J) = 2.007e-18 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 79\n",
       " Updating solution error estimates\n",
       "\n",
       "It 79/100: t = 3.950000e-01 ns (elapsed time = 3.48e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.463803e-06\n",
       "  1 KSP residual norm ||r||_B = 3.181286e-06\n",
       "  2 KSP residual norm ||r||_B = 1.355939e-06\n",
       "  3 KSP residual norm ||r||_B = 6.527058e-07\n",
       "  4 KSP residual norm ||r||_B = 3.715106e-07\n",
       "  5 KSP residual norm ||r||_B = 3.131958e-07\n",
       "  6 KSP residual norm ||r||_B = 3.335908e-07\n",
       "  7 KSP residual norm ||r||_B = 2.083998e-07\n",
       "  8 KSP residual norm ||r||_B = 1.173456e-07\n",
       "  9 KSP residual norm ||r||_B = 1.132518e-07\n",
       " 10 KSP residual norm ||r||_B = 2.412012e-07\n",
       " 11 KSP residual norm ||r||_B = 5.064276e-07\n",
       " 12 KSP residual norm ||r||_B = 3.433924e-07\n",
       " 13 KSP residual norm ||r||_B = 1.530079e-07\n",
       " 14 KSP residual norm ||r||_B = 5.986909e-08\n",
       " 15 KSP residual norm ||r||_B = 3.476772e-08\n",
       " 16 KSP residual norm ||r||_B = 2.379506e-08\n",
       " 17 KSP residual norm ||r||_B = 1.163482e-08\n",
       " 18 KSP residual norm ||r||_B = 3.353899e-09\n",
       " 19 KSP residual norm ||r||_B = 7.372886e-10\n",
       " 20 KSP residual norm ||r||_B = 1.592675e-10\n",
       " 21 KSP residual norm ||r||_B = 3.476687e-11\n",
       " 22 KSP residual norm ||r||_B = 7.380042e-12\n",
       " 23 KSP residual norm ||r||_B = 1.421321e-12\n",
       " 24 KSP residual norm ||r||_B = 3.088541e-13\n",
       " 25 KSP residual norm ||r||_B = 7.561506e-14\n",
       " 26 KSP residual norm ||r||_B = 1.601972e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.743e-01)\n",
       " Sol. ||E|| = 6.044257e-02, ||B|| = 1.204383e-03\n",
       " Field energy E (4.438e-19 J) + H (9.214e-19 J) = 1.365e-18 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 80/100: t = 4.000000e-01 ns (elapsed time = 3.52e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.625021e-06\n",
       "  1 KSP residual norm ||r||_B = 3.228631e-06\n",
       "  2 KSP residual norm ||r||_B = 1.378230e-06\n",
       "  3 KSP residual norm ||r||_B = 6.824159e-07\n",
       "  4 KSP residual norm ||r||_B = 4.129207e-07\n",
       "  5 KSP residual norm ||r||_B = 3.590761e-07\n",
       "  6 KSP residual norm ||r||_B = 3.480107e-07\n",
       "  7 KSP residual norm ||r||_B = 1.873366e-07\n",
       "  8 KSP residual norm ||r||_B = 8.679992e-08\n",
       "  9 KSP residual norm ||r||_B = 5.803127e-08\n",
       " 10 KSP residual norm ||r||_B = 9.207397e-08\n",
       " 11 KSP residual norm ||r||_B = 1.984762e-07\n",
       " 12 KSP residual norm ||r||_B = 2.185341e-07\n",
       " 13 KSP residual norm ||r||_B = 1.996023e-07\n",
       " 14 KSP residual norm ||r||_B = 1.619799e-07\n",
       " 15 KSP residual norm ||r||_B = 1.046489e-07\n",
       " 16 KSP residual norm ||r||_B = 3.988505e-08\n",
       " 17 KSP residual norm ||r||_B = 1.330054e-08\n",
       " 18 KSP residual norm ||r||_B = 3.466881e-09\n",
       " 19 KSP residual norm ||r||_B = 7.542854e-10\n",
       " 20 KSP residual norm ||r||_B = 1.627715e-10\n",
       " 21 KSP residual norm ||r||_B = 3.543604e-11\n",
       " 22 KSP residual norm ||r||_B = 7.521019e-12\n",
       " 23 KSP residual norm ||r||_B = 1.454383e-12\n",
       " 24 KSP residual norm ||r||_B = 3.166198e-13\n",
       " 25 KSP residual norm ||r||_B = 7.719842e-14\n",
       " 26 KSP residual norm ||r||_B = 1.635950e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.741e-01)\n",
       " Sol. ||E|| = 4.800818e-02, ||B|| = 9.572765e-04\n",
       " Field energy E (2.800e-19 J) + H (5.821e-19 J) = 8.621e-19 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 81\n",
       " Updating solution error estimates\n",
       "\n",
       "It 81/100: t = 4.050000e-01 ns (elapsed time = 3.57e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.674143e-06\n",
       "  1 KSP residual norm ||r||_B = 3.230851e-06\n",
       "  2 KSP residual norm ||r||_B = 1.373308e-06\n",
       "  3 KSP residual norm ||r||_B = 6.659163e-07\n",
       "  4 KSP residual norm ||r||_B = 3.830719e-07\n",
       "  5 KSP residual norm ||r||_B = 3.176082e-07\n",
       "  6 KSP residual norm ||r||_B = 3.156676e-07\n",
       "  7 KSP residual norm ||r||_B = 1.751806e-07\n",
       "  8 KSP residual norm ||r||_B = 7.225528e-08\n",
       "  9 KSP residual norm ||r||_B = 3.072699e-08\n",
       " 10 KSP residual norm ||r||_B = 2.763526e-08\n",
       " 11 KSP residual norm ||r||_B = 5.169164e-08\n",
       " 12 KSP residual norm ||r||_B = 7.454480e-08\n",
       " 13 KSP residual norm ||r||_B = 8.795523e-08\n",
       " 14 KSP residual norm ||r||_B = 9.671277e-08\n",
       " 15 KSP residual norm ||r||_B = 8.600105e-08\n",
       " 16 KSP residual norm ||r||_B = 3.833337e-08\n",
       " 17 KSP residual norm ||r||_B = 1.321637e-08\n",
       " 18 KSP residual norm ||r||_B = 3.480185e-09\n",
       " 19 KSP residual norm ||r||_B = 7.580359e-10\n",
       " 20 KSP residual norm ||r||_B = 1.635385e-10\n",
       " 21 KSP residual norm ||r||_B = 3.567077e-11\n",
       " 22 KSP residual norm ||r||_B = 7.579737e-12\n",
       " 23 KSP residual norm ||r||_B = 1.462445e-12\n",
       " 24 KSP residual norm ||r||_B = 3.177232e-13\n",
       " 25 KSP residual norm ||r||_B = 7.768176e-14\n",
       " 26 KSP residual norm ||r||_B = 1.647652e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 3.697339e-02, ||B|| = 7.376606e-04\n",
       " Field energy E (1.661e-19 J) + H (3.457e-19 J) = 5.117e-19 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 82/100: t = 4.100000e-01 ns (elapsed time = 3.61e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.765143e-06\n",
       "  1 KSP residual norm ||r||_B = 3.249130e-06\n",
       "  2 KSP residual norm ||r||_B = 1.382153e-06\n",
       "  3 KSP residual norm ||r||_B = 6.792031e-07\n",
       "  4 KSP residual norm ||r||_B = 4.025136e-07\n",
       "  5 KSP residual norm ||r||_B = 3.407701e-07\n",
       "  6 KSP residual norm ||r||_B = 3.301017e-07\n",
       "  7 KSP residual norm ||r||_B = 1.759829e-07\n",
       "  8 KSP residual norm ||r||_B = 7.030415e-08\n",
       "  9 KSP residual norm ||r||_B = 2.485095e-08\n",
       " 10 KSP residual norm ||r||_B = 1.308683e-08\n",
       " 11 KSP residual norm ||r||_B = 1.299232e-08\n",
       " 12 KSP residual norm ||r||_B = 1.267375e-08\n",
       " 13 KSP residual norm ||r||_B = 1.490496e-08\n",
       " 14 KSP residual norm ||r||_B = 2.402175e-08\n",
       " 15 KSP residual norm ||r||_B = 4.320768e-08\n",
       " 16 KSP residual norm ||r||_B = 3.405139e-08\n",
       " 17 KSP residual norm ||r||_B = 1.319585e-08\n",
       " 18 KSP residual norm ||r||_B = 3.518286e-09\n",
       " 19 KSP residual norm ||r||_B = 7.670625e-10\n",
       " 20 KSP residual norm ||r||_B = 1.654288e-10\n",
       " 21 KSP residual norm ||r||_B = 3.606237e-11\n",
       " 22 KSP residual norm ||r||_B = 7.667360e-12\n",
       " 23 KSP residual norm ||r||_B = 1.481122e-12\n",
       " 24 KSP residual norm ||r||_B = 3.217494e-13\n",
       " 25 KSP residual norm ||r||_B = 7.858804e-14\n",
       " 26 KSP residual norm ||r||_B = 1.668055e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.741e-01)\n",
       " Sol. ||E|| = 2.773767e-02, ||B|| = 5.536783e-04\n",
       " Field energy E (9.346e-20 J) + H (1.947e-19 J) = 2.882e-19 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 83\n",
       " Updating solution error estimates\n",
       "\n",
       "It 83/100: t = 4.150000e-01 ns (elapsed time = 3.67e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.857610e-06\n",
       "  1 KSP residual norm ||r||_B = 3.269053e-06\n",
       "  2 KSP residual norm ||r||_B = 1.387745e-06\n",
       "  3 KSP residual norm ||r||_B = 6.794944e-07\n",
       "  4 KSP residual norm ||r||_B = 3.982642e-07\n",
       "  5 KSP residual norm ||r||_B = 3.320840e-07\n",
       "  6 KSP residual norm ||r||_B = 3.230446e-07\n",
       "  7 KSP residual norm ||r||_B = 1.762096e-07\n",
       "  8 KSP residual norm ||r||_B = 7.279456e-08\n",
       "  9 KSP residual norm ||r||_B = 2.843221e-08\n",
       " 10 KSP residual norm ||r||_B = 1.685070e-08\n",
       " 11 KSP residual norm ||r||_B = 1.278239e-08\n",
       " 12 KSP residual norm ||r||_B = 6.741938e-09\n",
       " 13 KSP residual norm ||r||_B = 5.417125e-09\n",
       " 14 KSP residual norm ||r||_B = 8.072878e-09\n",
       " 15 KSP residual norm ||r||_B = 1.825870e-08\n",
       " 16 KSP residual norm ||r||_B = 2.544249e-08\n",
       " 17 KSP residual norm ||r||_B = 1.280090e-08\n",
       " 18 KSP residual norm ||r||_B = 3.547023e-09\n",
       " 19 KSP residual norm ||r||_B = 7.754682e-10\n",
       " 20 KSP residual norm ||r||_B = 1.672119e-10\n",
       " 21 KSP residual norm ||r||_B = 3.646474e-11\n",
       " 22 KSP residual norm ||r||_B = 7.758284e-12\n",
       " 23 KSP residual norm ||r||_B = 1.498562e-12\n",
       " 24 KSP residual norm ||r||_B = 3.253271e-13\n",
       " 25 KSP residual norm ||r||_B = 7.949669e-14\n",
       " 26 KSP residual norm ||r||_B = 1.688341e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 2.035126e-02, ||B|| = 4.063937e-04\n",
       " Field energy E (5.031e-20 J) + H (1.049e-19 J) = 1.552e-19 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 84/100: t = 4.200000e-01 ns (elapsed time = 3.71e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 8.924662e-06\n",
       "  1 KSP residual norm ||r||_B = 3.278150e-06\n",
       "  2 KSP residual norm ||r||_B = 1.392641e-06\n",
       "  3 KSP residual norm ||r||_B = 6.861648e-07\n",
       "  4 KSP residual norm ||r||_B = 4.058597e-07\n",
       "  5 KSP residual norm ||r||_B = 3.383410e-07\n",
       "  6 KSP residual norm ||r||_B = 3.250443e-07\n",
       "  7 KSP residual norm ||r||_B = 1.777560e-07\n",
       "  8 KSP residual norm ||r||_B = 7.699894e-08\n",
       "  9 KSP residual norm ||r||_B = 3.479269e-08\n",
       " 10 KSP residual norm ||r||_B = 2.421891e-08\n",
       " 11 KSP residual norm ||r||_B = 1.677303e-08\n",
       " 12 KSP residual norm ||r||_B = 9.040483e-09\n",
       " 13 KSP residual norm ||r||_B = 9.920403e-09\n",
       " 14 KSP residual norm ||r||_B = 1.880913e-08\n",
       " 15 KSP residual norm ||r||_B = 3.907042e-08\n",
       " 16 KSP residual norm ||r||_B = 3.376930e-08\n",
       " 17 KSP residual norm ||r||_B = 1.336162e-08\n",
       " 18 KSP residual norm ||r||_B = 3.582881e-09\n",
       " 19 KSP residual norm ||r||_B = 7.819185e-10\n",
       " 20 KSP residual norm ||r||_B = 1.685205e-10\n",
       " 21 KSP residual norm ||r||_B = 3.675883e-11\n",
       " 22 KSP residual norm ||r||_B = 7.827567e-12\n",
       " 23 KSP residual norm ||r||_B = 1.512089e-12\n",
       " 24 KSP residual norm ||r||_B = 3.279934e-13\n",
       " 25 KSP residual norm ||r||_B = 8.016640e-14\n",
       " 26 KSP residual norm ||r||_B = 1.704037e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.742e-01)\n",
       " Sol. ||E|| = 1.465939e-02, ||B|| = 2.928402e-04\n",
       " Field energy E (2.611e-20 J) + H (5.448e-20 J) = 8.058e-20 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 85\n",
       " Updating solution error estimates\n",
       "\n",
       "It 85/100: t = 4.250000e-01 ns (elapsed time = 3.76e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.026855e-06\n",
       "  1 KSP residual norm ||r||_B = 3.300754e-06\n",
       "  2 KSP residual norm ||r||_B = 1.399838e-06\n",
       "  3 KSP residual norm ||r||_B = 6.913012e-07\n",
       "  4 KSP residual norm ||r||_B = 4.102179e-07\n",
       "  5 KSP residual norm ||r||_B = 3.407617e-07\n",
       "  6 KSP residual norm ||r||_B = 3.256272e-07\n",
       "  7 KSP residual norm ||r||_B = 1.795908e-07\n",
       "  8 KSP residual norm ||r||_B = 8.045919e-08\n",
       "  9 KSP residual norm ||r||_B = 3.940749e-08\n",
       " 10 KSP residual norm ||r||_B = 2.959357e-08\n",
       " 11 KSP residual norm ||r||_B = 2.095145e-08\n",
       " 12 KSP residual norm ||r||_B = 1.396778e-08\n",
       " 13 KSP residual norm ||r||_B = 2.073464e-08\n",
       " 14 KSP residual norm ||r||_B = 4.293196e-08\n",
       " 15 KSP residual norm ||r||_B = 6.853730e-08\n",
       " 16 KSP residual norm ||r||_B = 3.873529e-08\n",
       " 17 KSP residual norm ||r||_B = 1.370763e-08\n",
       " 18 KSP residual norm ||r||_B = 3.629586e-09\n",
       " 19 KSP residual norm ||r||_B = 7.916721e-10\n",
       " 20 KSP residual norm ||r||_B = 1.705679e-10\n",
       " 21 KSP residual norm ||r||_B = 3.719871e-11\n",
       " 22 KSP residual norm ||r||_B = 7.925413e-12\n",
       " 23 KSP residual norm ||r||_B = 1.532068e-12\n",
       " 24 KSP residual norm ||r||_B = 3.322770e-13\n",
       " 25 KSP residual norm ||r||_B = 8.118097e-14\n",
       " 26 KSP residual norm ||r||_B = 1.726458e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 1.041567e-02, ||B|| = 2.081014e-04\n",
       " Field energy E (1.318e-20 J) + H (2.751e-20 J) = 4.069e-20 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 86/100: t = 4.300000e-01 ns (elapsed time = 3.80e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.091456e-06\n",
       "  1 KSP residual norm ||r||_B = 3.309104e-06\n",
       "  2 KSP residual norm ||r||_B = 1.404490e-06\n",
       "  3 KSP residual norm ||r||_B = 6.965301e-07\n",
       "  4 KSP residual norm ||r||_B = 4.138173e-07\n",
       "  5 KSP residual norm ||r||_B = 3.398543e-07\n",
       "  6 KSP residual norm ||r||_B = 3.206877e-07\n",
       "  7 KSP residual norm ||r||_B = 1.799127e-07\n",
       "  8 KSP residual norm ||r||_B = 8.576946e-08\n",
       "  9 KSP residual norm ||r||_B = 4.639559e-08\n",
       " 10 KSP residual norm ||r||_B = 3.436604e-08\n",
       " 11 KSP residual norm ||r||_B = 1.968860e-08\n",
       " 12 KSP residual norm ||r||_B = 1.074200e-08\n",
       " 13 KSP residual norm ||r||_B = 1.408798e-08\n",
       " 14 KSP residual norm ||r||_B = 2.923811e-08\n",
       " 15 KSP residual norm ||r||_B = 5.434698e-08\n",
       " 16 KSP residual norm ||r||_B = 3.704759e-08\n",
       " 17 KSP residual norm ||r||_B = 1.369136e-08\n",
       " 18 KSP residual norm ||r||_B = 3.653440e-09\n",
       " 19 KSP residual norm ||r||_B = 7.976382e-10\n",
       " 20 KSP residual norm ||r||_B = 1.717913e-10\n",
       " 21 KSP residual norm ||r||_B = 3.748085e-11\n",
       " 22 KSP residual norm ||r||_B = 7.992750e-12\n",
       " 23 KSP residual norm ||r||_B = 1.544935e-12\n",
       " 24 KSP residual norm ||r||_B = 3.347585e-13\n",
       " 25 KSP residual norm ||r||_B = 8.182539e-14\n",
       " 26 KSP residual norm ||r||_B = 1.741667e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.743e-01)\n",
       " Sol. ||E|| = 7.341306e-03, ||B|| = 1.467023e-04\n",
       " Field energy E (6.547e-21 J) + H (1.367e-20 J) = 2.022e-20 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 87\n",
       " Updating solution error estimates\n",
       "\n",
       "It 87/100: t = 4.350000e-01 ns (elapsed time = 3.85e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.190115e-06\n",
       "  1 KSP residual norm ||r||_B = 3.329287e-06\n",
       "  2 KSP residual norm ||r||_B = 1.410824e-06\n",
       "  3 KSP residual norm ||r||_B = 7.025032e-07\n",
       "  4 KSP residual norm ||r||_B = 4.201835e-07\n",
       "  5 KSP residual norm ||r||_B = 3.444725e-07\n",
       "  6 KSP residual norm ||r||_B = 3.221984e-07\n",
       "  7 KSP residual norm ||r||_B = 1.815779e-07\n",
       "  8 KSP residual norm ||r||_B = 8.891195e-08\n",
       "  9 KSP residual norm ||r||_B = 4.989430e-08\n",
       " 10 KSP residual norm ||r||_B = 3.701051e-08\n",
       " 11 KSP residual norm ||r||_B = 2.075790e-08\n",
       " 12 KSP residual norm ||r||_B = 1.192254e-08\n",
       " 13 KSP residual norm ||r||_B = 1.686362e-08\n",
       " 14 KSP residual norm ||r||_B = 3.567390e-08\n",
       " 15 KSP residual norm ||r||_B = 6.210647e-08\n",
       " 16 KSP residual norm ||r||_B = 3.844411e-08\n",
       " 17 KSP residual norm ||r||_B = 1.388349e-08\n",
       " 18 KSP residual norm ||r||_B = 3.696520e-09\n",
       " 19 KSP residual norm ||r||_B = 8.071386e-10\n",
       " 20 KSP residual norm ||r||_B = 1.737850e-10\n",
       " 21 KSP residual norm ||r||_B = 3.790504e-11\n",
       " 22 KSP residual norm ||r||_B = 8.087391e-12\n",
       " 23 KSP residual norm ||r||_B = 1.564596e-12\n",
       " 24 KSP residual norm ||r||_B = 3.389947e-13\n",
       " 25 KSP residual norm ||r||_B = 8.281366e-14\n",
       " 26 KSP residual norm ||r||_B = 1.763581e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 5.176211e-03, ||B|| = 1.034132e-04\n",
       " Field energy E (3.255e-21 J) + H (6.794e-21 J) = 1.005e-20 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 88/100: t = 4.400000e-01 ns (elapsed time = 3.89e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.259149e-06\n",
       "  1 KSP residual norm ||r||_B = 3.339068e-06\n",
       "  2 KSP residual norm ||r||_B = 1.415839e-06\n",
       "  3 KSP residual norm ||r||_B = 7.079515e-07\n",
       "  4 KSP residual norm ||r||_B = 4.233807e-07\n",
       "  5 KSP residual norm ||r||_B = 3.419959e-07\n",
       "  6 KSP residual norm ||r||_B = 3.153753e-07\n",
       "  7 KSP residual norm ||r||_B = 1.813079e-07\n",
       "  8 KSP residual norm ||r||_B = 9.411519e-08\n",
       "  9 KSP residual norm ||r||_B = 5.612697e-08\n",
       " 10 KSP residual norm ||r||_B = 3.990559e-08\n",
       " 11 KSP residual norm ||r||_B = 1.921831e-08\n",
       " 12 KSP residual norm ||r||_B = 8.412223e-09\n",
       " 13 KSP residual norm ||r||_B = 8.714475e-09\n",
       " 14 KSP residual norm ||r||_B = 1.670133e-08\n",
       " 15 KSP residual norm ||r||_B = 3.612599e-08\n",
       " 16 KSP residual norm ||r||_B = 3.369167e-08\n",
       " 17 KSP residual norm ||r||_B = 1.372977e-08\n",
       " 18 KSP residual norm ||r||_B = 3.719709e-09\n",
       " 19 KSP residual norm ||r||_B = 8.134963e-10\n",
       " 20 KSP residual norm ||r||_B = 1.750979e-10\n",
       " 21 KSP residual norm ||r||_B = 3.820359e-11\n",
       " 22 KSP residual norm ||r||_B = 8.158053e-12\n",
       " 23 KSP residual norm ||r||_B = 1.578365e-12\n",
       " 24 KSP residual norm ||r||_B = 3.417115e-13\n",
       " 25 KSP residual norm ||r||_B = 8.350406e-14\n",
       " 26 KSP residual norm ||r||_B = 1.779705e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.745e-01)\n",
       " Sol. ||E|| = 3.688253e-03, ||B|| = 7.367496e-05\n",
       " Field energy E (1.653e-21 J) + H (3.448e-21 J) = 5.101e-21 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 89\n",
       " Updating solution error estimates\n",
       "\n",
       "It 89/100: t = 4.450000e-01 ns (elapsed time = 3.94e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.351331e-06\n",
       "  1 KSP residual norm ||r||_B = 3.356062e-06\n",
       "  2 KSP residual norm ||r||_B = 1.421082e-06\n",
       "  3 KSP residual norm ||r||_B = 7.137712e-07\n",
       "  4 KSP residual norm ||r||_B = 4.296005e-07\n",
       "  5 KSP residual norm ||r||_B = 3.456513e-07\n",
       "  6 KSP residual norm ||r||_B = 3.154464e-07\n",
       "  7 KSP residual norm ||r||_B = 1.825415e-07\n",
       "  8 KSP residual norm ||r||_B = 9.740815e-08\n",
       "  9 KSP residual norm ||r||_B = 5.955012e-08\n",
       " 10 KSP residual norm ||r||_B = 4.179980e-08\n",
       " 11 KSP residual norm ||r||_B = 1.965277e-08\n",
       " 12 KSP residual norm ||r||_B = 8.687119e-09\n",
       " 13 KSP residual norm ||r||_B = 9.244092e-09\n",
       " 14 KSP residual norm ||r||_B = 1.798607e-08\n",
       " 15 KSP residual norm ||r||_B = 3.846962e-08\n",
       " 16 KSP residual norm ||r||_B = 3.457471e-08\n",
       " 17 KSP residual norm ||r||_B = 1.389301e-08\n",
       " 18 KSP residual norm ||r||_B = 3.759544e-09\n",
       " 19 KSP residual norm ||r||_B = 8.223871e-10\n",
       " 20 KSP residual norm ||r||_B = 1.769563e-10\n",
       " 21 KSP residual norm ||r||_B = 3.859960e-11\n",
       " 22 KSP residual norm ||r||_B = 8.247214e-12\n",
       " 23 KSP residual norm ||r||_B = 1.596965e-12\n",
       " 24 KSP residual norm ||r||_B = 3.456961e-13\n",
       " 25 KSP residual norm ||r||_B = 8.443367e-14\n",
       " 26 KSP residual norm ||r||_B = 1.800474e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 2.693483e-03, ||B|| = 5.375528e-05\n",
       " Field energy E (8.814e-22 J) + H (1.836e-21 J) = 2.717e-21 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 90/100: t = 4.500000e-01 ns (elapsed time = 3.98e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.425074e-06\n",
       "  1 KSP residual norm ||r||_B = 3.366967e-06\n",
       "  2 KSP residual norm ||r||_B = 1.426033e-06\n",
       "  3 KSP residual norm ||r||_B = 7.194954e-07\n",
       "  4 KSP residual norm ||r||_B = 4.333190e-07\n",
       "  5 KSP residual norm ||r||_B = 3.435124e-07\n",
       "  6 KSP residual norm ||r||_B = 3.088519e-07\n",
       "  7 KSP residual norm ||r||_B = 1.820125e-07\n",
       "  8 KSP residual norm ||r||_B = 1.019489e-07\n",
       "  9 KSP residual norm ||r||_B = 6.467525e-08\n",
       " 10 KSP residual norm ||r||_B = 4.386388e-08\n",
       " 11 KSP residual norm ||r||_B = 1.897227e-08\n",
       " 12 KSP residual norm ||r||_B = 6.597985e-09\n",
       " 13 KSP residual norm ||r||_B = 4.432449e-09\n",
       " 14 KSP residual norm ||r||_B = 6.209865e-09\n",
       " 15 KSP residual norm ||r||_B = 1.437713e-08\n",
       " 16 KSP residual norm ||r||_B = 2.320749e-08\n",
       " 17 KSP residual norm ||r||_B = 1.317075e-08\n",
       " 18 KSP residual norm ||r||_B = 3.774027e-09\n",
       " 19 KSP residual norm ||r||_B = 8.291341e-10\n",
       " 20 KSP residual norm ||r||_B = 1.783759e-10\n",
       " 21 KSP residual norm ||r||_B = 3.891617e-11\n",
       " 22 KSP residual norm ||r||_B = 8.321370e-12\n",
       " 23 KSP residual norm ||r||_B = 1.611801e-12\n",
       " 24 KSP residual norm ||r||_B = 3.487013e-13\n",
       " 25 KSP residual norm ||r||_B = 8.517520e-14\n",
       " 26 KSP residual norm ||r||_B = 1.817602e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 2.042282e-03, ||B|| = 4.073798e-05\n",
       " Field energy E (5.067e-22 J) + H (1.054e-21 J) = 1.561e-21 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 91\n",
       " Updating solution error estimates\n",
       "\n",
       "It 91/100: t = 4.550000e-01 ns (elapsed time = 4.03e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.511752e-06\n",
       "  1 KSP residual norm ||r||_B = 3.381344e-06\n",
       "  2 KSP residual norm ||r||_B = 1.430394e-06\n",
       "  3 KSP residual norm ||r||_B = 7.250267e-07\n",
       "  4 KSP residual norm ||r||_B = 4.389080e-07\n",
       "  5 KSP residual norm ||r||_B = 3.455021e-07\n",
       "  6 KSP residual norm ||r||_B = 3.070248e-07\n",
       "  7 KSP residual norm ||r||_B = 1.826126e-07\n",
       "  8 KSP residual norm ||r||_B = 1.052434e-07\n",
       "  9 KSP residual norm ||r||_B = 6.801249e-08\n",
       " 10 KSP residual norm ||r||_B = 4.541782e-08\n",
       " 11 KSP residual norm ||r||_B = 1.931341e-08\n",
       " 12 KSP residual norm ||r||_B = 6.796219e-09\n",
       " 13 KSP residual norm ||r||_B = 4.771155e-09\n",
       " 14 KSP residual norm ||r||_B = 6.985226e-09\n",
       " 15 KSP residual norm ||r||_B = 1.625866e-08\n",
       " 16 KSP residual norm ||r||_B = 2.485445e-08\n",
       " 17 KSP residual norm ||r||_B = 1.342015e-08\n",
       " 18 KSP residual norm ||r||_B = 3.813075e-09\n",
       " 19 KSP residual norm ||r||_B = 8.374983e-10\n",
       " 20 KSP residual norm ||r||_B = 1.801127e-10\n",
       " 21 KSP residual norm ||r||_B = 3.928758e-11\n",
       " 22 KSP residual norm ||r||_B = 8.405809e-12\n",
       " 23 KSP residual norm ||r||_B = 1.629454e-12\n",
       " 24 KSP residual norm ||r||_B = 3.524570e-13\n",
       " 25 KSP residual norm ||r||_B = 8.605375e-14\n",
       " 26 KSP residual norm ||r||_B = 1.837374e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 1.629078e-03, ||B|| = 3.244431e-05\n",
       " Field energy E (3.224e-22 J) + H (6.687e-22 J) = 9.911e-22 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 92/100: t = 4.600000e-01 ns (elapsed time = 4.07e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.588490e-06\n",
       "  1 KSP residual norm ||r||_B = 3.392530e-06\n",
       "  2 KSP residual norm ||r||_B = 1.434796e-06\n",
       "  3 KSP residual norm ||r||_B = 7.306859e-07\n",
       "  4 KSP residual norm ||r||_B = 4.430347e-07\n",
       "  5 KSP residual norm ||r||_B = 3.438703e-07\n",
       "  6 KSP residual norm ||r||_B = 3.010232e-07\n",
       "  7 KSP residual norm ||r||_B = 1.818410e-07\n",
       "  8 KSP residual norm ||r||_B = 1.089173e-07\n",
       "  9 KSP residual norm ||r||_B = 7.200038e-08\n",
       " 10 KSP residual norm ||r||_B = 4.694518e-08\n",
       " 11 KSP residual norm ||r||_B = 1.919849e-08\n",
       " 12 KSP residual norm ||r||_B = 5.935994e-09\n",
       " 13 KSP residual norm ||r||_B = 2.648314e-09\n",
       " 14 KSP residual norm ||r||_B = 2.081564e-09\n",
       " 15 KSP residual norm ||r||_B = 3.698396e-09\n",
       " 16 KSP residual norm ||r||_B = 8.775037e-09\n",
       " 17 KSP residual norm ||r||_B = 1.033313e-08\n",
       " 18 KSP residual norm ||r||_B = 3.765176e-09\n",
       " 19 KSP residual norm ||r||_B = 8.439240e-10\n",
       " 20 KSP residual norm ||r||_B = 1.815993e-10\n",
       " 21 KSP residual norm ||r||_B = 3.961521e-11\n",
       " 22 KSP residual norm ||r||_B = 8.482060e-12\n",
       " 23 KSP residual norm ||r||_B = 1.645054e-12\n",
       " 24 KSP residual norm ||r||_B = 3.556774e-13\n",
       " 25 KSP residual norm ||r||_B = 8.683013e-14\n",
       " 26 KSP residual norm ||r||_B = 1.855177e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.746e-01)\n",
       " Sol. ||E|| = 1.370890e-03, ||B|| = 2.728955e-05\n",
       " Field energy E (2.283e-22 J) + H (4.730e-22 J) = 7.014e-22 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 93\n",
       " Updating solution error estimates\n",
       "\n",
       "It 93/100: t = 4.650000e-01 ns (elapsed time = 4.12e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.671394e-06\n",
       "  1 KSP residual norm ||r||_B = 3.404975e-06\n",
       "  2 KSP residual norm ||r||_B = 1.438391e-06\n",
       "  3 KSP residual norm ||r||_B = 7.359069e-07\n",
       "  4 KSP residual norm ||r||_B = 4.480195e-07\n",
       "  5 KSP residual norm ||r||_B = 3.444001e-07\n",
       "  6 KSP residual norm ||r||_B = 2.976356e-07\n",
       "  7 KSP residual norm ||r||_B = 1.817011e-07\n",
       "  8 KSP residual norm ||r||_B = 1.118466e-07\n",
       "  9 KSP residual norm ||r||_B = 7.494361e-08\n",
       " 10 KSP residual norm ||r||_B = 4.815626e-08\n",
       " 11 KSP residual norm ||r||_B = 1.947040e-08\n",
       " 12 KSP residual norm ||r||_B = 6.079128e-09\n",
       " 13 KSP residual norm ||r||_B = 2.888680e-09\n",
       " 14 KSP residual norm ||r||_B = 2.575987e-09\n",
       " 15 KSP residual norm ||r||_B = 4.993361e-09\n",
       " 16 KSP residual norm ||r||_B = 1.138044e-08\n",
       " 17 KSP residual norm ||r||_B = 1.133126e-08\n",
       " 18 KSP residual norm ||r||_B = 3.825887e-09\n",
       " 19 KSP residual norm ||r||_B = 8.521544e-10\n",
       " 20 KSP residual norm ||r||_B = 1.832529e-10\n",
       " 21 KSP residual norm ||r||_B = 3.996901e-11\n",
       " 22 KSP residual norm ||r||_B = 8.563125e-12\n",
       " 23 KSP residual norm ||r||_B = 1.662075e-12\n",
       " 24 KSP residual norm ||r||_B = 3.592837e-13\n",
       " 25 KSP residual norm ||r||_B = 8.767392e-14\n",
       " 26 KSP residual norm ||r||_B = 1.874269e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.747e-01)\n",
       " Sol. ||E|| = 1.216471e-03, ||B|| = 2.417454e-05\n",
       " Field energy E (1.798e-22 J) + H (3.712e-22 J) = 5.510e-22 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 94/100: t = 4.700000e-01 ns (elapsed time = 4.16e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.749426e-06\n",
       "  1 KSP residual norm ||r||_B = 3.415777e-06\n",
       "  2 KSP residual norm ||r||_B = 1.441959e-06\n",
       "  3 KSP residual norm ||r||_B = 7.412096e-07\n",
       "  4 KSP residual norm ||r||_B = 4.522405e-07\n",
       "  5 KSP residual norm ||r||_B = 3.429644e-07\n",
       "  6 KSP residual norm ||r||_B = 2.920035e-07\n",
       "  7 KSP residual norm ||r||_B = 1.806034e-07\n",
       "  8 KSP residual norm ||r||_B = 1.146411e-07\n",
       "  9 KSP residual norm ||r||_B = 7.793585e-08\n",
       " 10 KSP residual norm ||r||_B = 4.926679e-08\n",
       " 11 KSP residual norm ||r||_B = 1.957990e-08\n",
       " 12 KSP residual norm ||r||_B = 5.852548e-09\n",
       " 13 KSP residual norm ||r||_B = 2.180175e-09\n",
       " 14 KSP residual norm ||r||_B = 9.679151e-10\n",
       " 15 KSP residual norm ||r||_B = 8.920004e-10\n",
       " 16 KSP residual norm ||r||_B = 1.848834e-09\n",
       " 17 KSP residual norm ||r||_B = 4.264862e-09\n",
       " 18 KSP residual norm ||r||_B = 3.393785e-09\n",
       " 19 KSP residual norm ||r||_B = 8.540960e-10\n",
       " 20 KSP residual norm ||r||_B = 1.847272e-10\n",
       " 21 KSP residual norm ||r||_B = 4.030012e-11\n",
       " 22 KSP residual norm ||r||_B = 8.640065e-12\n",
       " 23 KSP residual norm ||r||_B = 1.678099e-12\n",
       " 24 KSP residual norm ||r||_B = 3.626325e-13\n",
       " 25 KSP residual norm ||r||_B = 8.846777e-14\n",
       " 26 KSP residual norm ||r||_B = 1.892401e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.747e-01)\n",
       " Sol. ||E|| = 1.124033e-03, ||B|| = 2.233948e-05\n",
       " Field energy E (1.535e-22 J) + H (3.170e-22 J) = 4.705e-22 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 95\n",
       " Updating solution error estimates\n",
       "\n",
       "It 95/100: t = 4.750000e-01 ns (elapsed time = 4.21e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.829905e-06\n",
       "  1 KSP residual norm ||r||_B = 3.426753e-06\n",
       "  2 KSP residual norm ||r||_B = 1.444775e-06\n",
       "  3 KSP residual norm ||r||_B = 7.460463e-07\n",
       "  4 KSP residual norm ||r||_B = 4.567251e-07\n",
       "  5 KSP residual norm ||r||_B = 3.424305e-07\n",
       "  6 KSP residual norm ||r||_B = 2.875603e-07\n",
       "  7 KSP residual norm ||r||_B = 1.797335e-07\n",
       "  8 KSP residual norm ||r||_B = 1.169438e-07\n",
       "  9 KSP residual norm ||r||_B = 8.030048e-08\n",
       " 10 KSP residual norm ||r||_B = 5.015959e-08\n",
       " 11 KSP residual norm ||r||_B = 1.979156e-08\n",
       " 12 KSP residual norm ||r||_B = 5.928128e-09\n",
       " 13 KSP residual norm ||r||_B = 2.260704e-09\n",
       " 14 KSP residual norm ||r||_B = 1.126946e-09\n",
       " 15 KSP residual norm ||r||_B = 1.249125e-09\n",
       " 16 KSP residual norm ||r||_B = 2.832859e-09\n",
       " 17 KSP residual norm ||r||_B = 5.825208e-09\n",
       " 18 KSP residual norm ||r||_B = 3.603954e-09\n",
       " 19 KSP residual norm ||r||_B = 8.640519e-10\n",
       " 20 KSP residual norm ||r||_B = 1.863456e-10\n",
       " 21 KSP residual norm ||r||_B = 4.064201e-11\n",
       " 22 KSP residual norm ||r||_B = 8.718800e-12\n",
       " 23 KSP residual norm ||r||_B = 1.694748e-12\n",
       " 24 KSP residual norm ||r||_B = 3.661571e-13\n",
       " 25 KSP residual norm ||r||_B = 8.928984e-14\n",
       " 26 KSP residual norm ||r||_B = 1.911062e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.747e-01)\n",
       " Sol. ||E|| = 1.073096e-03, ||B|| = 2.129746e-05\n",
       " Field energy E (1.399e-22 J) + H (2.881e-22 J) = 4.281e-22 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 96/100: t = 4.800000e-01 ns (elapsed time = 4.25e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.908089e-06\n",
       "  1 KSP residual norm ||r||_B = 3.436795e-06\n",
       "  2 KSP residual norm ||r||_B = 1.447386e-06\n",
       "  3 KSP residual norm ||r||_B = 7.508160e-07\n",
       "  4 KSP residual norm ||r||_B = 4.607960e-07\n",
       "  5 KSP residual norm ||r||_B = 3.409021e-07\n",
       "  6 KSP residual norm ||r||_B = 2.820297e-07\n",
       "  7 KSP residual norm ||r||_B = 1.782272e-07\n",
       "  8 KSP residual norm ||r||_B = 1.189023e-07\n",
       "  9 KSP residual norm ||r||_B = 8.246538e-08\n",
       " 10 KSP residual norm ||r||_B = 5.094413e-08\n",
       " 11 KSP residual norm ||r||_B = 1.995846e-08\n",
       " 12 KSP residual norm ||r||_B = 5.925372e-09\n",
       " 13 KSP residual norm ||r||_B = 2.129528e-09\n",
       " 14 KSP residual norm ||r||_B = 7.609822e-10\n",
       " 15 KSP residual norm ||r||_B = 4.018929e-10\n",
       " 16 KSP residual norm ||r||_B = 5.159902e-10\n",
       " 17 KSP residual norm ||r||_B = 1.274268e-09\n",
       " 18 KSP residual norm ||r||_B = 2.344155e-09\n",
       " 19 KSP residual norm ||r||_B = 8.479259e-10\n",
       " 20 KSP residual norm ||r||_B = 1.876361e-10\n",
       " 21 KSP residual norm ||r||_B = 4.097010e-11\n",
       " 22 KSP residual norm ||r||_B = 8.795446e-12\n",
       " 23 KSP residual norm ||r||_B = 1.710952e-12\n",
       " 24 KSP residual norm ||r||_B = 3.695706e-13\n",
       " 25 KSP residual norm ||r||_B = 9.008880e-14\n",
       " 26 KSP residual norm ||r||_B = 1.929277e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.748e-01)\n",
       " Sol. ||E|| = 1.043363e-03, ||B|| = 2.071974e-05\n",
       " Field energy E (1.323e-22 J) + H (2.727e-22 J) = 4.050e-22 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 97\n",
       " Updating solution error estimates\n",
       "\n",
       "It 97/100: t = 4.850000e-01 ns (elapsed time = 4.30e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 9.986945e-06\n",
       "  1 KSP residual norm ||r||_B = 3.446558e-06\n",
       "  2 KSP residual norm ||r||_B = 1.449352e-06\n",
       "  3 KSP residual norm ||r||_B = 7.551572e-07\n",
       "  4 KSP residual norm ||r||_B = 4.648452e-07\n",
       "  5 KSP residual norm ||r||_B = 3.396313e-07\n",
       "  6 KSP residual norm ||r||_B = 2.769358e-07\n",
       "  7 KSP residual norm ||r||_B = 1.766952e-07\n",
       "  8 KSP residual norm ||r||_B = 1.204643e-07\n",
       "  9 KSP residual norm ||r||_B = 8.420793e-08\n",
       " 10 KSP residual norm ||r||_B = 5.157157e-08\n",
       " 11 KSP residual norm ||r||_B = 2.013381e-08\n",
       " 12 KSP residual norm ||r||_B = 5.971917e-09\n",
       " 13 KSP residual norm ||r||_B = 2.131659e-09\n",
       " 14 KSP residual norm ||r||_B = 7.243809e-10\n",
       " 15 KSP residual norm ||r||_B = 2.994449e-10\n",
       " 16 KSP residual norm ||r||_B = 2.662890e-10\n",
       " 17 KSP residual norm ||r||_B = 5.620577e-10\n",
       " 18 KSP residual norm ||r||_B = 1.464975e-09\n",
       " 19 KSP residual norm ||r||_B = 8.169404e-10\n",
       " 20 KSP residual norm ||r||_B = 1.887613e-10\n",
       " 21 KSP residual norm ||r||_B = 4.129838e-11\n",
       " 22 KSP residual norm ||r||_B = 8.872397e-12\n",
       " 23 KSP residual norm ||r||_B = 1.727383e-12\n",
       " 24 KSP residual norm ||r||_B = 3.730546e-13\n",
       " 25 KSP residual norm ||r||_B = 9.089670e-14\n",
       " 26 KSP residual norm ||r||_B = 1.947651e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.748e-01)\n",
       " Sol. ||E|| = 1.029410e-03, ||B|| = 2.041954e-05\n",
       " Field energy E (1.288e-22 J) + H (2.649e-22 J) = 3.936e-22 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 98/100: t = 4.900000e-01 ns (elapsed time = 4.33e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.006465e-05\n",
       "  1 KSP residual norm ||r||_B = 3.455676e-06\n",
       "  2 KSP residual norm ||r||_B = 1.450970e-06\n",
       "  3 KSP residual norm ||r||_B = 7.592917e-07\n",
       "  4 KSP residual norm ||r||_B = 4.686235e-07\n",
       "  5 KSP residual norm ||r||_B = 3.378552e-07\n",
       "  6 KSP residual norm ||r||_B = 2.713448e-07\n",
       "  7 KSP residual norm ||r||_B = 1.747316e-07\n",
       "  8 KSP residual norm ||r||_B = 1.216329e-07\n",
       "  9 KSP residual norm ||r||_B = 8.568063e-08\n",
       " 10 KSP residual norm ||r||_B = 5.209905e-08\n",
       " 11 KSP residual norm ||r||_B = 2.030043e-08\n",
       " 12 KSP residual norm ||r||_B = 6.026463e-09\n",
       " 13 KSP residual norm ||r||_B = 2.161700e-09\n",
       " 14 KSP residual norm ||r||_B = 7.681641e-10\n",
       " 15 KSP residual norm ||r||_B = 3.975105e-10\n",
       " 16 KSP residual norm ||r||_B = 4.990509e-10\n",
       " 17 KSP residual norm ||r||_B = 1.223290e-09\n",
       " 18 KSP residual norm ||r||_B = 2.317721e-09\n",
       " 19 KSP residual norm ||r||_B = 8.605772e-10\n",
       " 20 KSP residual norm ||r||_B = 1.906989e-10\n",
       " 21 KSP residual norm ||r||_B = 4.162928e-11\n",
       " 22 KSP residual norm ||r||_B = 8.948272e-12\n",
       " 23 KSP residual norm ||r||_B = 1.743620e-12\n",
       " 24 KSP residual norm ||r||_B = 3.764941e-13\n",
       " 25 KSP residual norm ||r||_B = 9.169339e-14\n",
       " 26 KSP residual norm ||r||_B = 1.965802e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.748e-01)\n",
       " Sol. ||E|| = 1.020722e-03, ||B|| = 2.026424e-05\n",
       " Field energy E (1.266e-22 J) + H (2.608e-22 J) = 3.874e-22 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 99\n",
       " Updating solution error estimates\n",
       "\n",
       "It 99/100: t = 4.950000e-01 ns (elapsed time = 4.39e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.014228e-05\n",
       "  1 KSP residual norm ||r||_B = 3.464361e-06\n",
       "  2 KSP residual norm ||r||_B = 1.452024e-06\n",
       "  3 KSP residual norm ||r||_B = 7.630282e-07\n",
       "  4 KSP residual norm ||r||_B = 4.722611e-07\n",
       "  5 KSP residual norm ||r||_B = 3.360650e-07\n",
       "  6 KSP residual norm ||r||_B = 2.658597e-07\n",
       "  7 KSP residual norm ||r||_B = 1.726144e-07\n",
       "  8 KSP residual norm ||r||_B = 1.224365e-07\n",
       "  9 KSP residual norm ||r||_B = 8.682926e-08\n",
       " 10 KSP residual norm ||r||_B = 5.250683e-08\n",
       " 11 KSP residual norm ||r||_B = 2.045502e-08\n",
       " 12 KSP residual norm ||r||_B = 6.072849e-09\n",
       " 13 KSP residual norm ||r||_B = 2.165731e-09\n",
       " 14 KSP residual norm ||r||_B = 7.368192e-10\n",
       " 15 KSP residual norm ||r||_B = 3.080099e-10\n",
       " 16 KSP residual norm ||r||_B = 2.808289e-10\n",
       " 17 KSP residual norm ||r||_B = 6.003143e-10\n",
       " 18 KSP residual norm ||r||_B = 1.538920e-09\n",
       " 19 KSP residual norm ||r||_B = 8.338548e-10\n",
       " 20 KSP residual norm ||r||_B = 1.918461e-10\n",
       " 21 KSP residual norm ||r||_B = 4.195068e-11\n",
       " 22 KSP residual norm ||r||_B = 9.023753e-12\n",
       " 23 KSP residual norm ||r||_B = 1.759908e-12\n",
       " 24 KSP residual norm ||r||_B = 3.799566e-13\n",
       " 25 KSP residual norm ||r||_B = 9.249045e-14\n",
       " 26 KSP residual norm ||r||_B = 1.983946e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.749e-01)\n",
       " Sol. ||E|| = 1.018367e-03, ||B|| = 2.019722e-05\n",
       " Field energy E (1.260e-22 J) + H (2.591e-22 J) = 3.851e-22 J\n",
       " Updating solution error estimates\n",
       "\n",
       "It 100/100: t = 5.000000e-01 ns (elapsed time = 4.42e+03 s)\n",
       "\n",
       "  Residual norms for PCG solve\n",
       "  0 KSP residual norm ||r||_B = 1.021921e-05\n",
       "  1 KSP residual norm ||r||_B = 3.472518e-06\n",
       "  2 KSP residual norm ||r||_B = 1.452650e-06\n",
       "  3 KSP residual norm ||r||_B = 7.664625e-07\n",
       "  4 KSP residual norm ||r||_B = 4.756760e-07\n",
       "  5 KSP residual norm ||r||_B = 3.339954e-07\n",
       "  6 KSP residual norm ||r||_B = 2.601473e-07\n",
       "  7 KSP residual norm ||r||_B = 1.701813e-07\n",
       "  8 KSP residual norm ||r||_B = 1.228588e-07\n",
       "  9 KSP residual norm ||r||_B = 8.770754e-08\n",
       " 10 KSP residual norm ||r||_B = 5.282285e-08\n",
       " 11 KSP residual norm ||r||_B = 2.060635e-08\n",
       " 12 KSP residual norm ||r||_B = 6.137182e-09\n",
       " 13 KSP residual norm ||r||_B = 2.224058e-09\n",
       " 14 KSP residual norm ||r||_B = 8.567606e-10\n",
       " 15 KSP residual norm ||r||_B = 5.817366e-10\n",
       " 16 KSP residual norm ||r||_B = 9.737037e-10\n",
       " 17 KSP residual norm ||r||_B = 2.446884e-09\n",
       " 18 KSP residual norm ||r||_B = 3.064676e-09\n",
       " 19 KSP residual norm ||r||_B = 8.910068e-10\n",
       " 20 KSP residual norm ||r||_B = 1.939059e-10\n",
       " 21 KSP residual norm ||r||_B = 4.227748e-11\n",
       " 22 KSP residual norm ||r||_B = 9.098501e-12\n",
       " 23 KSP residual norm ||r||_B = 1.776096e-12\n",
       " 24 KSP residual norm ||r||_B = 3.834005e-13\n",
       " 25 KSP residual norm ||r||_B = 9.328076e-14\n",
       " 26 KSP residual norm ||r||_B = 2.001950e-14\n",
       "PCG solver converged in 26 iterations (avg. reduction factor: 4.749e-01)\n",
       " Sol. ||E|| = 1.015768e-03, ||B|| = 2.016402e-05\n",
       " Field energy E (1.254e-22 J) + H (2.583e-22 J) = 3.836e-22 J\n",
       "\n",
       " Wrote fields to disk (Paraview) at step 101\n",
       " Updating solution error estimates\n",
       "\n",
       "Completed 0 iterations of adaptive mesh refinement (AMR):\n",
       " Indicator norm = 2.155e-01, global unknowns = 546784\n",
       " Max. iterations = 0, tol. = 1.000e-02\n",
       "\n",
       "Estimated peak per-rank memory usage is: Min. 2.5G, Max. 2.5G, Avg. 2.5G, Total 2.5G\n",
       "Estimated peak per-node memory usage is: Min. 2.5G, Max. 2.5G, Avg. 2.5G, Total 2.5G\n",
       "\n",
       "Elapsed Time Report (s)           Min.        Max.        Avg.\n",
       "==============================================================\n",
       "Initialization                   0.264       0.264       0.264\n",
       "  Mesh Preprocessing             1.036       1.036       1.036\n",
       "Operator Construction            0.698       0.698       0.698\n",
       "Linear Solve                   393.221     393.221     393.221\n",
       "  Setup                         15.687      15.687      15.687\n",
       "  Preconditioner              2882.904    2882.904    2882.904\n",
       "  Coarse Solve                 110.918     110.918     110.918\n",
       "Time Stepping                   21.993      21.993      21.993\n",
       "Estimation                       7.956       7.956       7.956\n",
       "  Construction                  12.551      12.551      12.551\n",
       "  Solve                        460.751     460.751     460.751\n",
       "Postprocessing                   9.454       9.454       9.454\n",
       "  Paraview                     574.700     574.700     574.700\n",
       "Disk IO                          0.310       0.310       0.310\n",
       "--------------------------------------------------------------\n",
       "Total                         4492.713    4492.713    4492.713\n",
       "\n",
       "Peak Memory                   Per-Node       Total   Total HWM\n",
       "==============================================================\n",
       "Initialization                    1.8M        1.8M        1.8M\n",
       "  Mesh Preprocessing             40.9M       40.9M       42.7M\n",
       "Operator Construction           419.3M      419.3M      462.0M\n",
       "Linear Solve                      0.0K        0.0K      462.0M\n",
       "  Setup                         601.7M      601.7M        1.0G\n",
       "  Preconditioner                  0.0K        0.0K        1.0G\n",
       "  Coarse Solve                    0.0K        0.0K        1.0G\n",
       "Time Stepping                   384.9M      384.9M        1.4G\n",
       "Estimation                      272.7M      272.7M        1.7G\n",
       "  Construction                  378.8M      378.8M        2.1G\n",
       "  Solve                         223.3M      223.3M        2.3G\n",
       "Postprocessing                  124.5M      124.5M        2.4G\n",
       "  Paraview                       25.6M       25.6M        2.4G\n",
       "Disk IO                          28.6M       28.6M        2.4G\n",
       "--------------------------------------------------------------\n",
       "Total                             2.5G        2.5G        2.5G
" ], "text/plain": [ "" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "from palacetoolkit.simulation import run_palace\n", "\n", "# Transient sim\n", "run_palace(config_file=\"l_antenna_transient.json\", num_procs=1)" ] }, { "cell_type": "markdown", "execution_count": null, "id": "40e271db", "metadata": { "papermill": { "duration": 0.00589, "end_time": "2026-08-04T15:58:21.655170+00:00", "exception": false, "start_time": "2026-08-04T15:58:21.649280+00:00", "status": "completed" }, "tags": [] }, "outputs": [], "source": [ "### Time domain simulation" ] }, { "cell_type": "markdown", "id": "a1570835", "metadata": { "tags": [ "papermill-error-cell-tag" ] }, "source": [ "Execution using papermill encountered an exception here and stopped:" ] }, { "cell_type": "code", "execution_count": 10, "id": "020674a7", "metadata": { "execution": { "iopub.execute_input": "2026-08-04T15:58:21.667704Z", "iopub.status.busy": "2026-08-04T15:58:21.667498Z", "iopub.status.idle": "2026-08-04T15:58:23.946990Z", "shell.execute_reply": "2026-08-04T15:58:23.946206Z" }, "papermill": { "duration": 2.286813, "end_time": "2026-08-04T15:58:23.947761+00:00", "exception": true, "start_time": "2026-08-04T15:58:21.660948+00:00", "status": "failed" }, "tags": [] }, "outputs": [ { "name": "stdout", "output_type": "stream", "text": [ "Computing global field range (excluding air box)...\n" ] }, { "name": "stdout", "output_type": "stream", "text": [ "Global max |E|: 7.5595e+06\n", "Rendering 51 frames at 10 fps...\n" ] }, { "ename": "ModuleNotFoundError", "evalue": "Install imageio to use `open_gif` with:\n\n pip install imageio", "output_type": "error", "traceback": [ "\u001b[31m---------------------------------------------------------------------------\u001b[39m", "\u001b[31mModuleNotFoundError\u001b[39m Traceback (most recent call last)", "\u001b[36mCell\u001b[39m\u001b[36m \u001b[39m\u001b[32mIn[10]\u001b[39m\u001b[32m, line 3\u001b[39m\n\u001b[32m 1\u001b[39m \u001b[38;5;28;01mfrom\u001b[39;00m palacetoolkit.postpro_vtu \u001b[38;5;28;01mimport\u001b[39;00m generate_transient_video\n\u001b[32m 2\u001b[39m \n\u001b[32m----> \u001b[39m\u001b[32m3\u001b[39m generate_transient_video(\n\u001b[32m 4\u001b[39m \u001b[33m\"postpro/l_antenna_transient\"\u001b[39m,\n\u001b[32m 5\u001b[39m \u001b[33m\"l_antenna.gif\"\u001b[39m,\n\u001b[32m 6\u001b[39m field_name=\u001b[33m\"E\"\u001b[39m, fps=\u001b[32m10\u001b[39m,\n", "\u001b[36mFile \u001b[39m\u001b[32m~/work/PalaceToolkit/PalaceToolkit/src/palacetoolkit/postpro_vtu.py:887\u001b[39m, in \u001b[36mgenerate_transient_video\u001b[39m\u001b[34m(postpro_dir, output_file, field_name, hidden_attrs, geometry_attrs, cmap, clim_scale, fps, window_size)\u001b[39m\n\u001b[32m 885\u001b[39m plotter = pv.Plotter(off_screen=\u001b[38;5;28;01mTrue\u001b[39;00m, window_size=window_size)\n\u001b[32m 886\u001b[39m plotter.set_background(\u001b[33m\"\u001b[39m\u001b[33mwhite\u001b[39m\u001b[33m\"\u001b[39m, top=\u001b[33m\"\u001b[39m\u001b[33mlightblue\u001b[39m\u001b[33m\"\u001b[39m)\n\u001b[32m--> \u001b[39m\u001b[32m887\u001b[39m \u001b[30;43mplotter\u001b[39;49m\u001b[30;43m.\u001b[39;49m\u001b[30;43mopen_gif\u001b[39;49m\u001b[30;43m(\u001b[39;49m\u001b[30;43mstr\u001b[39;49m\u001b[30;43m(\u001b[39;49m\u001b[30;43mout\u001b[39;49m\u001b[30;43m)\u001b[39;49m\u001b[30;43m,\u001b[39;49m\u001b[30;43m \u001b[39;49m\u001b[30;43mfps\u001b[39;49m\u001b[30;43m=\u001b[39;49m\u001b[30;43mfps\u001b[39;49m\u001b[30;43m)\u001b[39;49m\n\u001b[32m 889\u001b[39m \u001b[38;5;28;01mfor\u001b[39;00m idx \u001b[38;5;129;01min\u001b[39;00m selected:\n\u001b[32m 890\u001b[39m cdir = cycle_dirs[idx]\n", "\u001b[36mFile \u001b[39m\u001b[32m/opt/hostedtoolcache/Python/3.12.13/x64/lib/python3.12/site-packages/pyvista/_deprecate_positional_args.py:243\u001b[39m, in \u001b[36m_deprecate_positional_args.._inner_deprecate_positional_args..inner_f\u001b[39m\u001b[34m(*args, **kwargs)\u001b[39m\n\u001b[32m 239\u001b[39m warn_external(msg, PyVistaDeprecationWarning)\n\u001b[32m 241\u001b[39m warn_positional_args()\n\u001b[32m--> \u001b[39m\u001b[32m243\u001b[39m \u001b[38;5;28;01mreturn\u001b[39;00m \u001b[30;43mf\u001b[39;49m\u001b[30;43m(\u001b[39;49m\u001b[30;43m*\u001b[39;49m\u001b[30;43margs\u001b[39;49m\u001b[30;43m,\u001b[39;49m\u001b[30;43m \u001b[39;49m\u001b[30;43m*\u001b[39;49m\u001b[30;43m*\u001b[39;49m\u001b[30;43mkwargs\u001b[39;49m\u001b[30;43m)\u001b[39;49m\n", "\u001b[36mFile \u001b[39m\u001b[32m/opt/hostedtoolcache/Python/3.12.13/x64/lib/python3.12/site-packages/pyvista/plotting/plotter.py:5648\u001b[39m, in \u001b[36mBasePlotter.open_gif\u001b[39m\u001b[34m(self, filename, loop, fps, palettesize, subrectangles, **kwargs)\u001b[39m\n\u001b[32m 5646\u001b[39m \u001b[38;5;28;01mexcept\u001b[39;00m \u001b[38;5;167;01mModuleNotFoundError\u001b[39;00m: \u001b[38;5;66;03m# pragma: no cover\u001b[39;00m\n\u001b[32m 5647\u001b[39m msg = \u001b[33m'\u001b[39m\u001b[33mInstall imageio to use `open_gif` with:\u001b[39m\u001b[38;5;130;01m\\n\u001b[39;00m\u001b[38;5;130;01m\\n\u001b[39;00m\u001b[33m pip install imageio\u001b[39m\u001b[33m'\u001b[39m\n\u001b[32m-> \u001b[39m\u001b[32m5648\u001b[39m \u001b[38;5;28;01mraise\u001b[39;00m \u001b[38;5;167;01mModuleNotFoundError\u001b[39;00m(msg) \u001b[38;5;28;01mfrom\u001b[39;00m\u001b[38;5;250m \u001b[39m\u001b[38;5;28;01mNone\u001b[39;00m\n\u001b[32m 5650\u001b[39m filename = Path(filename)\n\u001b[32m 5651\u001b[39m \u001b[38;5;28;01mif\u001b[39;00m filename.suffix != \u001b[33m'\u001b[39m\u001b[33m.gif\u001b[39m\u001b[33m'\u001b[39m:\n", "\u001b[31mModuleNotFoundError\u001b[39m: Install imageio to use `open_gif` with:\n\n pip install imageio" ] } ], "source": [ "from palacetoolkit.postpro_vtu import generate_transient_video\n", "\n", "generate_transient_video(\n", " \"postpro/l_antenna_transient\",\n", " \"l_antenna.gif\",\n", " field_name=\"E\", fps=10,\n", ")" ] }, { "cell_type": "markdown", "execution_count": null, "id": "b97ce019", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "### Driven simulation\n", "\n", "We need to perform a driven type simulation to get the s parameters." ] }, { "cell_type": "code", "execution_count": null, "id": "2df4b9a0", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "run_palace(config_file=\"l_antenna_driven.json\", num_procs=1)" ] }, { "cell_type": "code", "execution_count": null, "id": "9cb2c556", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "# S parameters. Return the frequency where the minimum is reached.\n", "from pathlib import Path\n", "from palacetoolkit.postpro import s_params\n", "\n", "notebook_dir = Path().resolve()\n", "postpro_dir = notebook_dir / \"postpro\" / \"l_antenna_driven\"\n", "\n", "f = s_params(str(postpro_dir / \"port-S.csv\"))" ] }, { "cell_type": "markdown", "execution_count": null, "id": "chamfer_intro", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "### Chamfered L-Antenna\n", "\n", "Now repeat the analysis with a 45° chamfer (miter) at the inner corner of the bend.\n", "Chamfering a right-angle microstrip bend reduces the discontinuity capacitance,\n", "improving return loss and signal integrity at high frequencies.\n" ] }, { "cell_type": "code", "execution_count": null, "id": "chamfer_geom", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "chamfer: float = 0.6 * w3\n", "mesh_file_ch: str = \"l_antenna_chamfered.msh\"\n", "\n", "total_xmin = -l1/2 - air_margin\n", "total_xmax = l1/2 + air_margin\n", "total_ymin = -w1/2 - air_margin\n", "total_ymax = w1/2 + air_margin\n", "total_zmax = h + air_height\n", "\n", "gmsh.initialize()\n", "gmsh.model.add(\"patch_antenna_chamfered\")\n", "kernel = gmsh.model.occ\n", "\n", "c = chamfer\n", "poly_pts = [\n", " (-l1/2, -w3/2, h),\n", " (w3 - c, -w3/2, h),\n", " (w3, -w3/2 + c, h),\n", " (w3, w1/2, h),\n", " (0, w1/2, h),\n", " (0, w3/2, h),\n", " (-l1/2, w3/2, h),\n", "]\n", "pt_tags = [kernel.addPoint(x, y, z) for x, y, z in poly_pts]\n", "lines = []\n", "for i in range(len(pt_tags)):\n", " lines.append(kernel.addLine(pt_tags[i], pt_tags[(i+1) % len(pt_tags)]))\n", "loop = kernel.addCurveLoop(lines)\n", "top_conductor_ch = kernel.addPlaneSurface([loop])\n", "kernel.synchronize()\n", "\n", "substrate = kernel.addBox(-l1/2, -w1/2, 0, l1, w1, h)\n", "airsphere_radius = max(abs(total_xmin), abs(total_xmax),\n", " abs(total_ymin), abs(total_ymax), total_zmax)\n", "air_sphere = kernel.addSphere(0.0, 0.0, 0.0, airsphere_radius)\n", "ground_plane = kernel.addRectangle(-l1/2, -w1/2, 0, l1, w1)\n", "\n", "# Port 1 at x = -l1/2\n", "pa = kernel.addPoint(-l1/2, -w3/2, 0)\n", "pb = kernel.addPoint(-l1/2, w3/2, 0)\n", "pc = kernel.addPoint(-l1/2, w3/2, h)\n", "pd = kernel.addPoint(-l1/2, -w3/2, h)\n", "la = kernel.addLine(pa, pb)\n", "lb = kernel.addLine(pb, pc)\n", "lc = kernel.addLine(pc, pd)\n", "ld = kernel.addLine(pd, pa)\n", "loop1 = kernel.addCurveLoop([la, lb, lc, ld])\n", "lumped_port_1 = kernel.addPlaneSurface([loop1])\n", "\n", "# Port 2 at y = w1/2\n", "pe = kernel.addPoint(0, w1/2, 0)\n", "pf = kernel.addPoint(w3, w1/2, 0)\n", "pg = kernel.addPoint(w3, w1/2, h)\n", "ph = kernel.addPoint(0, w1/2, h)\n", "le = kernel.addLine(pe, pf)\n", "lf = kernel.addLine(pf, pg)\n", "lg = kernel.addLine(pg, ph)\n", "lh = kernel.addLine(ph, pe)\n", "loop2 = kernel.addCurveLoop([le, lf, lg, lh])\n", "lumped_port_2 = kernel.addPlaneSurface([loop2])\n", "kernel.synchronize()\n", "\n", "entities_ch = [\n", " Entity(\"substrate\", dim=3, btype=\"dielectric\", mesh_order=1,\n", " tags=[substrate], loss_tan=loss_tan, eps_r=eps_r, mu_r=1.0),\n", " Entity(\"air_sphere\", dim=3, btype=\"dielectric\", mesh_order=2,\n", " tags=[air_sphere], loss_tan=0.0, eps_r=1.0, mu_r=1.0),\n", " Entity(\"top_conductor\", dim=2, btype=\"pec\", mesh_order=1,\n", " tags=[top_conductor_ch]),\n", " Entity(\"ground_plane\", dim=2, btype=\"pec\", mesh_order=1, tags=[ground_plane]),\n", " Entity(\"lumped_port_1\", dim=2, btype=\"lumped_port\", mesh_order=0,\n", " tags=[lumped_port_1], R=50.0, direction=\"+Z\", excitation=True),\n", " Entity(\"lumped_port_2\", dim=2, btype=\"lumped_port\", mesh_order=0,\n", " tags=[lumped_port_2], R=50.0, direction=\"+Z\", excitation=False),\n", "]\n", "print(\"puto\")\n", "# Single fragment against 3D volumes (skips boolean cut pipeline)\n", "gmsh.model.occ.synchronize()\n", "dimtags_2d = [dt for e in entities_ch if e.dim == 2 for dt in e.dimtags]\n", "dimtags_3d = [dt for e in entities_ch if e.dim == 3 for dt in e.dimtags]\n", "_, out_map = gmsh.model.occ.fragment(\n", " dimtags_2d, dimtags_3d,\n", " removeObject=True, removeTool=True,\n", ")\n", "gmsh.model.occ.synchronize()\n", "\n", "# Update dimtags in same order as fragment call (2D first, then 3D)\n", "frag_order = [e for e in entities_ch if e.dim == 2] + [e for e in entities_ch if e.dim == 3]\n", "idx = 0\n", "for entity in frag_order:\n", " new_tags = []\n", " for _ in entity.dimtags:\n", " if idx < len(out_map):\n", " new_tags.extend(out_map[idx])\n", " idx += 1\n", " if new_tags:\n", " entity.dimtags = list(set(new_tags))\n", "\n", "# Direct physical groups\n", "# 3D volumes first, deduplicated by priority so the substrate keeps\n", "# its volume and the air_sphere only claims the remaining air.\n", "pg_map_ch = {}\n", "claimed_vols = set()\n", "for entity in sorted([e for e in entities_ch if e.dim == 3], key=lambda e: e.mesh_order):\n", " tags = [t for d, t in entity.dimtags if d == 3]\n", " unique = [t for t in tags if t not in claimed_vols]\n", " claimed_vols.update(unique)\n", " if unique:\n", " pg = gmsh.model.addPhysicalGroup(3, unique, name=entity.name)\n", " pg_map_ch[entity.name] = pg\n", "for entity in entities_ch:\n", " if entity.dim != 2:\n", " continue\n", " tags = sorted(set(t for d, t in entity.dimtags if d == entity.dim))\n", " if tags:\n", " pg = gmsh.model.addPhysicalGroup(entity.dim, tags, name=entity.name)\n", " pg_map_ch[entity.name] = pg\n", "\n", "# Interface surfaces between 3D volumes\n", "vol_ents = [e for e in entities_ch if e.dim == 3]\n", "surf_to_names = {}\n", "for ve in vol_ents:\n", " bnd = gmsh.model.getBoundary(\n", " ve.dimtags, combined=False, oriented=False, recursive=False\n", " )\n", " for d, t in bnd:\n", " if d == 2:\n", " atag = abs(t)\n", " up, _ = gmsh.model.getAdjacencies(2, atag)\n", " adj = {abs(s) for s in up if s > 0}\n", " names = set()\n", " for ve2 in vol_ents:\n", " if any(abs(vt) in adj for dd, vt in ve2.dimtags):\n", " names.add(ve2.name)\n", " surf_to_names.setdefault(atag, set()).update(names)\n", "\n", "assigned = {abs(t) for e in entities_ch if e.dim == 2\n", " for d, t in e.dimtags if d == 2}\n", "for stag, names in surf_to_names.items():\n", " if stag in assigned:\n", " continue\n", " slist = sorted(names)\n", " label = \"__\".join(slist) if len(slist) > 1 else f\"{slist[0]}__None\"\n", " if label not in pg_map_ch:\n", " pg = gmsh.model.addPhysicalGroup(2, [stag], name=label)\n", " pg_map_ch[label] = pg\n", "create_graded_mesh(wavelength,\n", " ppw_near=30,\n", " ppw_far=15,\n", " set_as_background=True,\n", " local_refinements={\n", " entities_ch[-1].dimtags[0]: 30,\n", " entities_ch[-2].dimtags[0]: 30\n", " })\n", "\n", "mesh_sizes_ch = {\n", " \"substrate\": wavelength / 12,\n", " \"air_sphere\": wavelength / 4,\n", " \"lumped_port_1\": wavelength / 18,\n", " \"lumped_port_2\": wavelength / 18,\n", " \"top_conductor\": wavelength / 10\n", "}\n", "\n", "generate_3d_mesh(entities_ch, mesh_sizes_ch, mesh_file_ch,\n", " optimize=True, verbose=False)\n", "gmsh.finalize()" ] }, { "cell_type": "code", "execution_count": null, "id": "5308ba4b", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "view_mesh(mesh_file_ch, transparent_groups= \"air_sphere__None\")" ] }, { "cell_type": "code", "execution_count": null, "id": "chamfer_configs", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "from palacetoolkit.simulation import generate_palace_config_from_entities\n", "\n", "output_file_transient_ch = \"l_antenna_chamfered_transient.json\"\n", "output_file_driven_ch = \"l_antenna_chamfered_driven.json\"\n", "\n", "config_transient_ch = generate_palace_config_from_entities(\n", " entity_defs=[e.to_dict() for e in entities_ch],\n", " pg_map=pg_map_ch,\n", " mesh_file=mesh_file_ch,\n", " output_file=output_file_transient_ch,\n", " sim_type=\"transient\",\n", " excitation_freq=freq,\n", " excitation_width=0.05,\n", " max_time=0.5,\n", " time_step=0.005,\n", " save_step=2,\n", ")\n", "\n", "config_driven_ch = generate_palace_config_from_entities(\n", " entity_defs=[e.to_dict() for e in entities_ch],\n", " pg_map=pg_map_ch,\n", " mesh_file=mesh_file_ch,\n", " output_file=output_file_driven_ch,\n", " sim_type=\"driven\",\n", " L0=1.0,\n", " solver_order=2,\n", " absorbing_order=1,\n", " farfield=False,\n", " freq_min=freq_min,\n", " freq_max=freq_max,\n", " freq_step=freq_step,\n", " linear_maxits=300,\n", ")" ] }, { "cell_type": "code", "execution_count": null, "id": "chamfer_run", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "from palacetoolkit.simulation import run_palace\n", "\n", "# Uncomment to run the simulations (may take hours each):\n", "# run_palace(config_file=output_file_transient_ch, num_procs=1)\n", "# run_palace(config_file=output_file_driven_ch, num_procs=1)" ] }, { "cell_type": "code", "execution_count": null, "id": "chamfer_transient_anim", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "from palacetoolkit.postpro_vtu import generate_transient_video\n", "\n", "# Uncomment after running the transient simulation:\n", "# generate_transient_video(\n", "# \"postpro/l_antenna_chamfered_transient\",\n", "# \"l_antenna_chamfered.gif\",\n", "# field_name=\"E\", fps=10,\n", "# )" ] }, { "cell_type": "code", "execution_count": null, "id": "chamfer_compare", "metadata": { "papermill": { "duration": null, "end_time": null, "exception": null, "start_time": null, "status": "pending" }, "tags": [] }, "outputs": [], "source": [ "import matplotlib.pyplot as plt\n", "import numpy as np\n", "from pathlib import Path\n", "\n", "notebook_dir = Path().resolve()\n", "base = notebook_dir / \"postpro\"\n", "\n", "def load_port_s(csv_path):\n", " data = np.loadtxt(csv_path, delimiter=\",\", skiprows=1)\n", " return data[:, 0], data[:, 1], data[:, 3] # freq, |S11|_dB, |S21|_dB\n", "\n", "f_orig, s11_orig, s21_orig = load_port_s(\n", " str(base / \"l_antenna_driven\" / \"port-S.csv\"))\n", "f_ch, s11_ch, s21_ch = load_port_s(\n", " str(base / \"l_antenna_chamfered_driven\" / \"port-S.csv\"))\n", "\n", "fig, (ax1, ax2) = plt.subplots(1, 2, figsize=(14, 5))\n", "\n", "ax1.plot(f_orig, s11_orig, \"b-^\", label=\"Original\", markersize=4)\n", "ax1.plot(f_ch, s11_ch, \"r-s\", label=\"Chamfered\", markersize=4)\n", "ax1.set_xlabel(\"Frequency (GHz)\")\n", "ax1.set_ylabel(\"|S11| (dB)\")\n", "ax1.set_title(\"Return Loss (S11) - lower is better\")\n", "ax1.legend()\n", "ax1.grid(True)\n", "\n", "ax2.plot(f_orig, s21_orig, \"b-^\", label=\"Original\", markersize=4)\n", "ax2.plot(f_ch, s21_ch, \"r-s\", label=\"Chamfered\", markersize=4)\n", "ax2.set_xlabel(\"Frequency (GHz)\")\n", "ax2.set_ylabel(\"|S21| (dB)\")\n", "ax2.set_title(\"Insertion Loss (S21) - higher is better\")\n", "ax2.legend()\n", "ax2.grid(True)\n", "\n", "plt.tight_layout()\n", "plt.show()\n", "\n", "idx_orig = np.argmin(s11_orig)\n", "idx_ch = np.argmin(s11_ch)\n", "print(f\"Original - min |S11| = {s11_orig[idx_orig]:.1f} dB @ {f_orig[idx_orig]:.3f} GHz\")\n", "print(f\"Chamfered - min |S11| = {s11_ch[idx_ch]:.1f} dB @ {f_ch[idx_ch]:.3f} GHz\")\n", "print(f\"|S21| at S11 min: original = {s21_orig[idx_orig]:.2f} dB, chamfered = {s21_ch[idx_ch]:.2f} dB\")" ] } ], "metadata": { "kernelspec": { "display_name": ".venv (3.12.3.final.0)", "language": "python", "name": "python3" }, "language_info": { "codemirror_mode": { "name": "ipython", "version": 3 }, "file_extension": ".py", "mimetype": "text/x-python", "name": "python", "nbconvert_exporter": "python", "pygments_lexer": "ipython3", "version": "3.12.13" }, "papermill": { "default_parameters": {}, "duration": 4505.081548, "end_time": "2026-08-04T15:58:24.569179+00:00", "environment_variables": {}, "exception": true, "input_path": "docs/examples/l_antenna.ipynb", "output_path": "docs/examples/l_antenna.ipynb", "parameters": {}, "start_time": "2026-08-04T14:43:19.487631+00:00", "version": "2.7.0" } }, "nbformat": 4, "nbformat_minor": 5 }