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已同步 2025-08-05 20:16:52 +08:00
233 行
11 KiB
Python
233 行
11 KiB
Python
# Copyright (C) 2015-2017: The University of Edinburgh
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# Authors: Craig Warren and Antonis Giannopoulos
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#
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# This file is part of gprMax.
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#
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# gprMax is free software: you can redistribute it and/or modify
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# it under the terms of the GNU General Public License as published by
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# the Free Software Foundation, either version 3 of the License, or
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# (at your option) any later version.
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#
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# gprMax is distributed in the hope that it will be useful,
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# but WITHOUT ANY WARRANTY; without even the implied warranty of
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# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
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# GNU General Public License for more details.
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#
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# You should have received a copy of the GNU General Public License
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# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
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import datetime
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import os
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import sys
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from time import perf_counter
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from colorama import init, Fore, Style
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init()
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import h5py
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import numpy as np
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np.seterr(invalid='raise')
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import matplotlib.pyplot as plt
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if sys.platform == 'linux':
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plt.switch_backend('agg')
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from gprMax.gprMax import api
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from gprMax.exceptions import GeneralError
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from tests.analytical_solutions import hertzian_dipole_fs
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"""Compare field outputs
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Usage:
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cd gprMax
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python -m tests.test_basic_suite
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"""
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basepath = os.path.join(os.path.dirname(os.path.abspath(__file__)), 'models_basic')
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# List of available test models
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testmodels = ['hertzian_dipole_fs_analytical', '2D_ExHyHz', '2D_EyHxHz', '2D_EzHxHy', 'cylinder_Ascan_2D', 'hertzian_dipole_fs', 'hertzian_dipole_hs', 'hertzian_dipole_dispersive']
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# Select a specific model if desired
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#testmodels = [testmodels[0], testmodels[1], testmodels[2], testmodels[3], testmodels[4], testmodels[5]]
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#testmodels = [testmodels[5]]
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testresults = dict.fromkeys(testmodels)
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path = '/rxs/rx1/'
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starttime = perf_counter()
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for i, model in enumerate(testmodels):
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testresults[model] = {}
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# Run model
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api(os.path.join(basepath, model + os.path.sep + model + '.in'))
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# Special case for analytical comparison
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if model == 'hertzian_dipole_fs_analytical':
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# Get output for model file
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filetest = h5py.File(os.path.join(basepath, model + os.path.sep + model + '.out'),'r')
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testresults[model]['Test version'] = filetest.attrs['gprMax']
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# Get available field output component names
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outputstest = list(filetest[path].keys())
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# Arrays for storing time
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floattype = filetest[path + outputstest[0]].dtype
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timetest = np.zeros((filetest.attrs['Iterations']), dtype=floattype)
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timetest = np.arange(0, filetest.attrs['dt'] * filetest.attrs['Iterations'], filetest.attrs['dt']) / 1e-9
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timeref = timetest
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# Arrays for storing field data
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datatest = np.zeros((filetest.attrs['Iterations'], len(outputstest)), dtype=floattype)
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print(datatest.shape)
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for ID, name in enumerate(outputstest):
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datatest[:,ID] = filetest[path + str(name)][:]
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# Tx/Rx position to feed to analytical solution
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rxpos = filetest[path].attrs['Position']
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txpos = filetest['/srcs/src1/'].attrs['Position']
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rxposrelative = ((rxpos[0] - txpos[0]), (rxpos[1] - txpos[1]), (rxpos[2] - txpos[2]))
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# Analytical solution of a dipole in free space
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dataref = hertzian_dipole_fs(filetest.attrs['Iterations'], filetest.attrs['dt'], filetest.attrs['dx, dy, dz'], rxposrelative)
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filetest.close()
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# Diffs
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datadiffs = np.zeros(datatest.shape, dtype=floattype)
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for i in range(len(outputstest)):
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max = np.amax(np.abs(dataref[:,i]))
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try:
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datadiffs[:,i] = ((np.abs(dataref[:,i] - datatest[:,i])) / max) * 100
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except FloatingPointError:
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print('FloatingPointError')
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datadiffs[:,i] = 0
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# Register test passed
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threshold = 2 # Percent
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if np.amax(np.amax(datadiffs)) < 2:
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testresults[model]['Pass'] = True
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else:
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testresults[model]['Pass'] = False
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testresults[model]['Max diff'] = np.amax(np.amax(datadiffs))
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else:
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# Get output for model and reference files
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fileref = h5py.File(os.path.join(basepath, model + os.path.sep + model + '_ref.out'),'r')
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filetest = h5py.File(os.path.join(basepath, model + os.path.sep + model + '.out'),'r')
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testresults[model]['Ref version'] = fileref.attrs['gprMax']
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testresults[model]['Test version'] = filetest.attrs['gprMax']
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# Get available field output component names
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outputsref = list(fileref[path].keys())
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outputstest = list(filetest[path].keys())
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if outputsref != outputstest:
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raise GeneralError('Field output components do not match reference solution')
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# Check that type of float used to store fields matches
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if filetest[path + outputstest[0]].dtype != fileref[path + outputsref[0]].dtype:
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raise GeneralError('Type of floating point number does not match reference solution')
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else:
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floattype = fileref[path + outputsref[0]].dtype
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# Array for storing time
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timeref = np.zeros((fileref.attrs['Iterations']), dtype=floattype)
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timeref = np.arange(0, fileref.attrs['dt'] * fileref.attrs['Iterations'], fileref.attrs['dt']) / 1e-9
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timetest = np.zeros((filetest.attrs['Iterations']), dtype=floattype)
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timetest = np.arange(0, filetest.attrs['dt'] * filetest.attrs['Iterations'], filetest.attrs['dt']) / 1e-9
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# Get available field output component names
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outputsref = list(fileref[path].keys())
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outputstest = list(filetest[path].keys())
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if outputsref != outputstest:
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raise GeneralError('Field output components do not match reference solution')
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# Arrays for storing field data
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dataref = np.zeros((fileref.attrs['Iterations'], len(outputsref)), dtype=floattype)
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datatest = np.zeros((filetest.attrs['Iterations'], len(outputstest)), dtype=floattype)
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for ID, name in enumerate(outputsref):
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dataref[:,ID] = fileref[path + str(name)][:]
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datatest[:,ID] = filetest[path + str(name)][:]
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fileref.close()
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filetest.close()
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# Diffs
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datadiffs = np.zeros(datatest.shape, dtype=floattype)
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for i in range(len(outputstest)):
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max = np.nanmax(np.abs(dataref[:,i]))
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try:
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datadiffs[:,i] = ((np.abs(dataref[:,i] - datatest[:,i])) / max) * 100
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except FloatingPointError:
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print('FloatingPointError')
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datadiffs[:,i] = 0
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# Register test passed
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if not np.any(datadiffs):
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testresults[model]['Pass'] = True
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else:
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testresults[model]['Pass'] = False
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testresults[model]['Max diff'] = np.amax(np.amax(datadiffs))
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# Plot datasets
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fig1, ((ex1, hx1), (ey1, hy1), (ez1, hz1)) = plt.subplots(nrows=3, ncols=2, sharex=False, sharey='col', subplot_kw=dict(xlabel='Time [ns]'), num=model + '.in', figsize=(20, 10), facecolor='w', edgecolor='w')
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ex1.plot(timetest, datatest[:,0],'r', lw=2, label=model)
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ex1.plot(timeref, dataref[:,0],'g', lw=2, ls='--', label=model + '(Ref)')
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ey1.plot(timetest, datatest[:,1],'r', lw=2, label=model)
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ey1.plot(timeref, dataref[:,1],'g', lw=2, ls='--', label=model + '(Ref)')
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ez1.plot(timetest, datatest[:,2],'r', lw=2, label=model)
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ez1.plot(timeref, dataref[:,2],'g', lw=2, ls='--', label=model + '(Ref)')
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hx1.plot(timetest, datatest[:,3],'r', lw=2, label=model)
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hx1.plot(timeref, dataref[:,3],'g', lw=2, ls='--', label=model + '(Ref)')
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hy1.plot(timetest, datatest[:,4],'r', lw=2, label=model)
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hy1.plot(timeref, dataref[:,4],'g', lw=2, ls='--', label=model + '(Ref)')
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hz1.plot(timetest, datatest[:,5],'r', lw=2, label=model)
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hz1.plot(timeref, dataref[:,5],'g', lw=2, ls='--', label=model + '(Ref)')
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ylabels = ['$E_x$, field strength [V/m]', '$H_x$, field strength [A/m]', '$E_y$, field strength [V/m]', '$H_y$, field strength [A/m]', '$E_z$, field strength [V/m]', '$H_z$, field strength [A/m]']
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for i, ax in enumerate(fig1.axes):
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ax.set_ylabel(ylabels[i])
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ax.set_xlim(0, np.amax(timetest))
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ax.grid()
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ax.legend()
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# Plot diffs
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fig2, ((ex2, hx2), (ey2, hy2), (ez2, hz2)) = plt.subplots(nrows=3, ncols=2, sharex=False, sharey='col', subplot_kw=dict(xlabel='Time [ns]'), num='Diffs: ' + model + '.in', figsize=(20, 10), facecolor='w', edgecolor='w')
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ex2.plot(timeref, datadiffs[:,0],'r', lw=2, label='Ex')
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ey2.plot(timeref, datadiffs[:,1],'r', lw=2, label='Ey')
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ez2.plot(timeref, datadiffs[:,2],'r', lw=2, label='Ez')
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hx2.plot(timeref, datadiffs[:,3],'r', lw=2, label='Hx')
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hy2.plot(timeref, datadiffs[:,4],'r', lw=2, label='Hy')
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hz2.plot(timeref, datadiffs[:,5],'r', lw=2, label='Hz')
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ylabels = ['$E_x$, difference [%]', '$H_x$, difference [%]', '$E_y$, difference [%]', '$H_y$, difference [%]', '$E_z$, difference [%]', '$H_z$, difference [%]']
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for i, ax in enumerate(fig2.axes):
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ax.set_ylabel(ylabels[i])
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ax.set_xlim(0, np.amax(timetest))
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ax.grid()
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# Save a PDF/PNG of the figure
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savename = os.path.join(basepath, model + os.path.sep + model)
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#fig1.savefig(savename + '.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
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#fig2.savefig(savename + '_diffs.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
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fig1.savefig(savename + '.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
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fig2.savefig(savename + '_diffs.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
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stoptime = perf_counter()
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# Summary of results
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passed = 0
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for name, data in testresults.items():
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if 'analytical' in name:
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if data['Pass']:
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print(Fore.GREEN + "Test '{}.in' using v.{} compared to analytical solution passed. Maximum difference = {}%".format(name, data['Test version'], data['Max diff']) + Style.RESET_ALL)
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passed += 1
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else:
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print(Fore.RED + "Test '{}.in' using v.{} compared to analytical solution failed. Maximum difference = {}%".format(name, data['Test version'], data['Max diff']) + Style.RESET_ALL)
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else:
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if data['Pass']:
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print(Fore.GREEN + "Test '{}.in' using v.{} compared to reference solution using v.{} passed. Maximum difference = {}%".format(name, data['Test version'], data['Ref version'], data['Max diff']) + Style.RESET_ALL)
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passed += 1
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else:
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print(Fore.RED + "Test '{}.in' using v.{} compared to reference solution using v.{} failed. Maximum difference = {}%".format(name, data['Test version'], data['Ref version'], data['Max diff']) + Style.RESET_ALL)
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print('{} of {} tests passed successfully in [HH:MM:SS]: {}'.format(passed, len(testmodels), datetime.timedelta(seconds=int(stoptime - starttime))))
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