Removing use_line_collection in plotting

use_line_collection is removed in matplotlib 3.8.0
这个提交包含在:
JingziC
2024-01-29 17:10:01 +09:00
提交者 GitHub
父节点 f27420e927
当前提交 cb5d26b433
共有 3 个文件被更改,包括 834 次插入834 次删除

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@@ -1,237 +1,237 @@
# Copyright (C) 2015-2023: The University of Edinburgh
# Authors: Craig Warren and Antonis Giannopoulos
#
# This file is part of gprMax.
#
# gprMax is free software: you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation, either version 3 of the License, or
# (at your option) any later version.
#
# gprMax is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
#
# You should have received a copy of the GNU General Public License
# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
import argparse
import os
import sys
import h5py
import numpy as np
import matplotlib.pyplot as plt
import matplotlib.gridspec as gridspec
from gprMax.exceptions import CmdInputError
from gprMax.receivers import Rx
from gprMax.utilities import fft_power
def mpl_plot(filename, outputs=Rx.defaultoutputs, fft=False):
"""Plots electric and magnetic fields and currents from all receiver points in the given output file. Each receiver point is plotted in a new figure window.
Args:
filename (string): Filename (including path) of output file.
outputs (list): List of field/current components to plot.
fft (boolean): Plot FFT switch.
Returns:
plt (object): matplotlib plot object.
"""
# Open output file and read some attributes
f = h5py.File(filename, 'r')
nrx = f.attrs['nrx']
dt = f.attrs['dt']
iterations = f.attrs['Iterations']
time = np.linspace(0, (iterations - 1) * dt, num=iterations)
# Check there are any receivers
if nrx == 0:
raise CmdInputError('No receivers found in {}'.format(filename))
# Check for single output component when doing a FFT
if fft:
if not len(outputs) == 1:
raise CmdInputError('A single output must be specified when using the -fft option')
# New plot for each receiver
for rx in range(1, nrx + 1):
path = '/rxs/rx' + str(rx) + '/'
availableoutputs = list(f[path].keys())
# If only a single output is required, create one subplot
if len(outputs) == 1:
# Check for polarity of output and if requested output is in file
if outputs[0][-1] == '-':
polarity = -1
outputtext = '-' + outputs[0][0:-1]
output = outputs[0][0:-1]
else:
polarity = 1
outputtext = outputs[0]
output = outputs[0]
if output not in availableoutputs:
raise CmdInputError('{} output requested to plot, but the available output for receiver 1 is {}'.format(output, ', '.join(availableoutputs)))
outputdata = f[path + output][:] * polarity
# Plotting if FFT required
if fft:
# FFT
freqs, power = fft_power(outputdata, dt)
freqmaxpower = np.where(np.isclose(power, 0))[0][0]
# Set plotting range to -60dB from maximum power or 4 times
# frequency at maximum power
try:
pltrange = np.where(power[freqmaxpower:] < -60)[0][0] + freqmaxpower + 1
except:
pltrange = freqmaxpower * 4
pltrange = np.s_[0:pltrange]
# Plot time history of output component
fig, (ax1, ax2) = plt.subplots(nrows=1, ncols=2, num='rx' + str(rx), figsize=(20, 10), facecolor='w', edgecolor='w')
line1 = ax1.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax1.set_xlabel('Time [s]')
ax1.set_ylabel(outputtext + ' field strength [V/m]')
ax1.set_xlim([0, np.amax(time)])
ax1.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra
markerline, stemlines, baseline = ax2.stem(freqs[pltrange], power[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
line2 = ax2.plot(freqs[pltrange], power[pltrange], 'r', lw=2)
ax2.set_xlabel('Frequency [Hz]')
ax2.set_ylabel('Power [dB]')
ax2.grid(which='both', axis='both', linestyle='-.')
# Change colours and labels for magnetic field components or currents
if 'H' in outputs[0]:
plt.setp(line1, color='g')
plt.setp(line2, color='g')
plt.setp(ax1, ylabel=outputtext + ' field strength [A/m]')
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
elif 'I' in outputs[0]:
plt.setp(line1, color='b')
plt.setp(line2, color='b')
plt.setp(ax1, ylabel=outputtext + ' current [A]')
plt.setp(stemlines, 'color', 'b')
plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
plt.show()
# Plotting if no FFT required
else:
fig, ax = plt.subplots(subplot_kw=dict(xlabel='Time [s]', ylabel=outputtext + ' field strength [V/m]'), num='rx' + str(rx), figsize=(20, 10), facecolor='w', edgecolor='w')
line = ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_xlim([0, np.amax(time)])
# ax.set_ylim([-15, 20])
ax.grid(which='both', axis='both', linestyle='-.')
if 'H' in output:
plt.setp(line, color='g')
plt.setp(ax, ylabel=outputtext + ', field strength [A/m]')
elif 'I' in output:
plt.setp(line, color='b')
plt.setp(ax, ylabel=outputtext + ', current [A]')
# If multiple outputs required, create all nine subplots and populate only the specified ones
else:
fig, ax = plt.subplots(subplot_kw=dict(xlabel='Time [s]'), num='rx' + str(rx), figsize=(20, 10), facecolor='w', edgecolor='w')
if len(outputs) == 9:
gs = gridspec.GridSpec(3, 3, hspace=0.3, wspace=0.3)
else:
gs = gridspec.GridSpec(3, 2, hspace=0.3, wspace=0.3)
for output in outputs:
# Check for polarity of output and if requested output is in file
if output[-1] == 'm':
polarity = -1
outputtext = '-' + output[0:-1]
output = output[0:-1]
else:
polarity = 1
outputtext = output
# Check if requested output is in file
if output not in availableoutputs:
raise CmdInputError('Output(s) requested to plot: {}, but available output(s) for receiver {} in the file: {}'.format(', '.join(outputs), rx, ', '.join(availableoutputs)))
outputdata = f[path + output][:] * polarity
if output == 'Ex':
ax = plt.subplot(gs[0, 0])
ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [V/m]')
# ax.set_ylim([-15, 20])
elif output == 'Ey':
ax = plt.subplot(gs[1, 0])
ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [V/m]')
# ax.set_ylim([-15, 20])
elif output == 'Ez':
ax = plt.subplot(gs[2, 0])
ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [V/m]')
# ax.set_ylim([-15, 20])
elif output == 'Hx':
ax = plt.subplot(gs[0, 1])
ax.plot(time, outputdata, 'g', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [A/m]')
# ax.set_ylim([-0.03, 0.03])
elif output == 'Hy':
ax = plt.subplot(gs[1, 1])
ax.plot(time, outputdata, 'g', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [A/m]')
# ax.set_ylim([-0.03, 0.03])
elif output == 'Hz':
ax = plt.subplot(gs[2, 1])
ax.plot(time, outputdata, 'g', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [A/m]')
# ax.set_ylim([-0.03, 0.03])
elif output == 'Ix':
ax = plt.subplot(gs[0, 2])
ax.plot(time, outputdata, 'b', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', current [A]')
elif output == 'Iy':
ax = plt.subplot(gs[1, 2])
ax.plot(time, outputdata, 'b', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', current [A]')
elif output == 'Iz':
ax = plt.subplot(gs[2, 2])
ax.plot(time, outputdata, 'b', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', current [A]')
for ax in fig.axes:
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Save a PDF/PNG of the figure
# fig.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_rx' + str(rx) + '.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
# fig.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_rx' + str(rx) + '.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
f.close()
return plt
if __name__ == "__main__":
# Parse command line arguments
parser = argparse.ArgumentParser(description='Plots electric and magnetic fields and currents from all receiver points in the given output file. Each receiver point is plotted in a new figure window.', usage='cd gprMax; python -m tools.plot_Ascan outputfile')
parser.add_argument('outputfile', help='name of output file including path')
parser.add_argument('--outputs', help='outputs to be plotted', default=Rx.defaultoutputs, choices=['Ex', 'Ey', 'Ez', 'Hx', 'Hy', 'Hz', 'Ix', 'Iy', 'Iz', 'Ex-', 'Ey-', 'Ez-', 'Hx-', 'Hy-', 'Hz-', 'Ix-', 'Iy-', 'Iz-'], nargs='+')
parser.add_argument('-fft', action='store_true', help='plot FFT (single output must be specified)', default=False)
args = parser.parse_args()
plthandle = mpl_plot(args.outputfile, args.outputs, fft=args.fft)
plthandle.show()
# Copyright (C) 2015-2023: The University of Edinburgh
# Authors: Craig Warren and Antonis Giannopoulos
#
# This file is part of gprMax.
#
# gprMax is free software: you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation, either version 3 of the License, or
# (at your option) any later version.
#
# gprMax is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
#
# You should have received a copy of the GNU General Public License
# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
import argparse
import os
import sys
import h5py
import numpy as np
import matplotlib.pyplot as plt
import matplotlib.gridspec as gridspec
from gprMax.exceptions import CmdInputError
from gprMax.receivers import Rx
from gprMax.utilities import fft_power
def mpl_plot(filename, outputs=Rx.defaultoutputs, fft=False):
"""Plots electric and magnetic fields and currents from all receiver points in the given output file. Each receiver point is plotted in a new figure window.
Args:
filename (string): Filename (including path) of output file.
outputs (list): List of field/current components to plot.
fft (boolean): Plot FFT switch.
Returns:
plt (object): matplotlib plot object.
"""
# Open output file and read some attributes
f = h5py.File(filename, 'r')
nrx = f.attrs['nrx']
dt = f.attrs['dt']
iterations = f.attrs['Iterations']
time = np.linspace(0, (iterations - 1) * dt, num=iterations)
# Check there are any receivers
if nrx == 0:
raise CmdInputError('No receivers found in {}'.format(filename))
# Check for single output component when doing a FFT
if fft:
if not len(outputs) == 1:
raise CmdInputError('A single output must be specified when using the -fft option')
# New plot for each receiver
for rx in range(1, nrx + 1):
path = '/rxs/rx' + str(rx) + '/'
availableoutputs = list(f[path].keys())
# If only a single output is required, create one subplot
if len(outputs) == 1:
# Check for polarity of output and if requested output is in file
if outputs[0][-1] == '-':
polarity = -1
outputtext = '-' + outputs[0][0:-1]
output = outputs[0][0:-1]
else:
polarity = 1
outputtext = outputs[0]
output = outputs[0]
if output not in availableoutputs:
raise CmdInputError('{} output requested to plot, but the available output for receiver 1 is {}'.format(output, ', '.join(availableoutputs)))
outputdata = f[path + output][:] * polarity
# Plotting if FFT required
if fft:
# FFT
freqs, power = fft_power(outputdata, dt)
freqmaxpower = np.where(np.isclose(power, 0))[0][0]
# Set plotting range to -60dB from maximum power or 4 times
# frequency at maximum power
try:
pltrange = np.where(power[freqmaxpower:] < -60)[0][0] + freqmaxpower + 1
except:
pltrange = freqmaxpower * 4
pltrange = np.s_[0:pltrange]
# Plot time history of output component
fig, (ax1, ax2) = plt.subplots(nrows=1, ncols=2, num='rx' + str(rx), figsize=(20, 10), facecolor='w', edgecolor='w')
line1 = ax1.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax1.set_xlabel('Time [s]')
ax1.set_ylabel(outputtext + ' field strength [V/m]')
ax1.set_xlim([0, np.amax(time)])
ax1.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra
markerline, stemlines, baseline = ax2.stem(freqs[pltrange], power[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
line2 = ax2.plot(freqs[pltrange], power[pltrange], 'r', lw=2)
ax2.set_xlabel('Frequency [Hz]')
ax2.set_ylabel('Power [dB]')
ax2.grid(which='both', axis='both', linestyle='-.')
# Change colours and labels for magnetic field components or currents
if 'H' in outputs[0]:
plt.setp(line1, color='g')
plt.setp(line2, color='g')
plt.setp(ax1, ylabel=outputtext + ' field strength [A/m]')
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
elif 'I' in outputs[0]:
plt.setp(line1, color='b')
plt.setp(line2, color='b')
plt.setp(ax1, ylabel=outputtext + ' current [A]')
plt.setp(stemlines, 'color', 'b')
plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
plt.show()
# Plotting if no FFT required
else:
fig, ax = plt.subplots(subplot_kw=dict(xlabel='Time [s]', ylabel=outputtext + ' field strength [V/m]'), num='rx' + str(rx), figsize=(20, 10), facecolor='w', edgecolor='w')
line = ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_xlim([0, np.amax(time)])
# ax.set_ylim([-15, 20])
ax.grid(which='both', axis='both', linestyle='-.')
if 'H' in output:
plt.setp(line, color='g')
plt.setp(ax, ylabel=outputtext + ', field strength [A/m]')
elif 'I' in output:
plt.setp(line, color='b')
plt.setp(ax, ylabel=outputtext + ', current [A]')
# If multiple outputs required, create all nine subplots and populate only the specified ones
else:
fig, ax = plt.subplots(subplot_kw=dict(xlabel='Time [s]'), num='rx' + str(rx), figsize=(20, 10), facecolor='w', edgecolor='w')
if len(outputs) == 9:
gs = gridspec.GridSpec(3, 3, hspace=0.3, wspace=0.3)
else:
gs = gridspec.GridSpec(3, 2, hspace=0.3, wspace=0.3)
for output in outputs:
# Check for polarity of output and if requested output is in file
if output[-1] == 'm':
polarity = -1
outputtext = '-' + output[0:-1]
output = output[0:-1]
else:
polarity = 1
outputtext = output
# Check if requested output is in file
if output not in availableoutputs:
raise CmdInputError('Output(s) requested to plot: {}, but available output(s) for receiver {} in the file: {}'.format(', '.join(outputs), rx, ', '.join(availableoutputs)))
outputdata = f[path + output][:] * polarity
if output == 'Ex':
ax = plt.subplot(gs[0, 0])
ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [V/m]')
# ax.set_ylim([-15, 20])
elif output == 'Ey':
ax = plt.subplot(gs[1, 0])
ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [V/m]')
# ax.set_ylim([-15, 20])
elif output == 'Ez':
ax = plt.subplot(gs[2, 0])
ax.plot(time, outputdata, 'r', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [V/m]')
# ax.set_ylim([-15, 20])
elif output == 'Hx':
ax = plt.subplot(gs[0, 1])
ax.plot(time, outputdata, 'g', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [A/m]')
# ax.set_ylim([-0.03, 0.03])
elif output == 'Hy':
ax = plt.subplot(gs[1, 1])
ax.plot(time, outputdata, 'g', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [A/m]')
# ax.set_ylim([-0.03, 0.03])
elif output == 'Hz':
ax = plt.subplot(gs[2, 1])
ax.plot(time, outputdata, 'g', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', field strength [A/m]')
# ax.set_ylim([-0.03, 0.03])
elif output == 'Ix':
ax = plt.subplot(gs[0, 2])
ax.plot(time, outputdata, 'b', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', current [A]')
elif output == 'Iy':
ax = plt.subplot(gs[1, 2])
ax.plot(time, outputdata, 'b', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', current [A]')
elif output == 'Iz':
ax = plt.subplot(gs[2, 2])
ax.plot(time, outputdata, 'b', lw=2, label=outputtext)
ax.set_ylabel(outputtext + ', current [A]')
for ax in fig.axes:
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Save a PDF/PNG of the figure
# fig.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_rx' + str(rx) + '.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
# fig.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_rx' + str(rx) + '.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
f.close()
return plt
if __name__ == "__main__":
# Parse command line arguments
parser = argparse.ArgumentParser(description='Plots electric and magnetic fields and currents from all receiver points in the given output file. Each receiver point is plotted in a new figure window.', usage='cd gprMax; python -m tools.plot_Ascan outputfile')
parser.add_argument('outputfile', help='name of output file including path')
parser.add_argument('--outputs', help='outputs to be plotted', default=Rx.defaultoutputs, choices=['Ex', 'Ey', 'Ez', 'Hx', 'Hy', 'Hz', 'Ix', 'Iy', 'Iz', 'Ex-', 'Ey-', 'Ez-', 'Hx-', 'Hy-', 'Hz-', 'Ix-', 'Iy-', 'Iz-'], nargs='+')
parser.add_argument('-fft', action='store_true', help='plot FFT (single output must be specified)', default=False)
args = parser.parse_args()
plthandle = mpl_plot(args.outputfile, args.outputs, fft=args.fft)
plthandle.show()

查看文件

@@ -1,424 +1,424 @@
# Copyright (C) 2015-2023: The University of Edinburgh
# Authors: Craig Warren and Antonis Giannopoulos
#
# This file is part of gprMax.
#
# gprMax is free software: you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation, either version 3 of the License, or
# (at your option) any later version.
#
# gprMax is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
#
# You should have received a copy of the GNU General Public License
# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
import argparse
import os
import sys
import h5py
import numpy as np
import matplotlib.pyplot as plt
import matplotlib.gridspec as gridspec
from gprMax.exceptions import CmdInputError
def calculate_antenna_params(filename, tltxnumber=1, tlrxnumber=None, rxnumber=None, rxcomponent=None):
"""Calculates antenna parameters - incident, reflected and total volatges and currents; s11, (s21) and input impedance.
Args:
filename (string): Filename (including path) of output file.
tltxnumber (int): Transmitter antenna - transmission line number
tlrxnumber (int): Receiver antenna - transmission line number
rxnumber (int): Receiver antenna - output number
rxcomponent (str): Receiver antenna - output electric field component
Returns:
antennaparams (dict): Antenna parameters.
"""
# Open output file and read some attributes
f = h5py.File(filename, 'r')
dxdydz = f.attrs['dx_dy_dz']
dt = f.attrs['dt']
iterations = f.attrs['Iterations']
# Calculate time array and frequency bin spacing
time = np.linspace(0, (iterations - 1) * dt, num=iterations)
df = 1 / np.amax(time)
print('Time window: {:g} s ({} iterations)'.format(np.amax(time), iterations))
print('Time step: {:g} s'.format(dt))
print('Frequency bin spacing: {:g} Hz'.format(df))
# Read/calculate voltages and currents from transmitter antenna
tltxpath = '/tls/tl' + str(tltxnumber) + '/'
# Incident voltages/currents
Vinc = f[tltxpath + 'Vinc'][:]
Iinc = f[tltxpath + 'Iinc'][:]
# Total (incident + reflected) voltages/currents
Vtotal = f[tltxpath + 'Vtotal'][:]
Itotal = f[tltxpath + 'Itotal'][:]
# Reflected voltages/currents
Vref = Vtotal - Vinc
Iref = Itotal - Iinc
# If a receiver antenna is used (with a transmission line or receiver), get received voltage for s21
if tlrxnumber:
tlrxpath = '/tls/tl' + str(tlrxnumber) + '/'
Vrec = f[tlrxpath + 'Vtotal'][:]
elif rxnumber:
rxpath = '/rxs/rx' + str(rxnumber) + '/'
availableoutputs = list(f[rxpath].keys())
if rxcomponent not in availableoutputs:
raise CmdInputError('{} output requested, but the available output for receiver {} is {}'.format(rxcomponent, rxnumber, ', '.join(availableoutputs)))
rxpath += rxcomponent
# Received voltage
if rxcomponent == 'Ex':
Vrec = f[rxpath][:] * -1 * dxdydz[0]
elif rxcomponent == 'Ey':
Vrec = f[rxpath][:] * -1 * dxdydz[1]
elif rxcomponent == 'Ez':
Vrec = f[rxpath][:] * -1 * dxdydz[2]
f.close()
# Frequency bins
freqs = np.fft.fftfreq(Vinc.size, d=dt)
# Delay correction - current lags voltage, so delay voltage to match current timestep
delaycorrection = np.exp(1j * 2 * np.pi * freqs * (dt / 2))
# Calculate s11 and (optionally) s21
with np.errstate(divide='ignore'):
s11 = np.abs(np.fft.fft(Vref) / np.fft.fft(Vinc))
if tlrxnumber or rxnumber:
with np.errstate(divide='ignore'):
s21 = np.abs(np.fft.fft(Vrec) / np.fft.fft(Vinc))
# Calculate input impedance
with np.errstate(divide='ignore'):
zin = (np.fft.fft(Vtotal) * delaycorrection) / np.fft.fft(Itotal)
# Calculate input admittance
with np.errstate(divide='ignore'):
yin = np.fft.fft(Itotal) / (np.fft.fft(Vtotal) * delaycorrection)
# Convert to decibels (ignore warning from taking a log of any zero values)
with np.errstate(divide='ignore'):
Vincp = 20 * np.log10(np.abs((np.fft.fft(Vinc) * delaycorrection)))
Iincp = 20 * np.log10(np.abs(np.fft.fft(Iinc)))
Vrefp = 20 * np.log10(np.abs((np.fft.fft(Vref) * delaycorrection)))
Irefp = 20 * np.log10(np.abs(np.fft.fft(Iref)))
Vtotalp = 20 * np.log10(np.abs((np.fft.fft(Vtotal) * delaycorrection)))
Itotalp = 20 * np.log10(np.abs(np.fft.fft(Itotal)))
s11 = 20 * np.log10(s11)
# Replace any NaNs or Infs from zero division
Vincp[np.invert(np.isfinite(Vincp))] = 0
Iincp[np.invert(np.isfinite(Iincp))] = 0
Vrefp[np.invert(np.isfinite(Vrefp))] = 0
Irefp[np.invert(np.isfinite(Irefp))] = 0
Vtotalp[np.invert(np.isfinite(Vtotalp))] = 0
Itotalp[np.invert(np.isfinite(Itotalp))] = 0
s11[np.invert(np.isfinite(s11))] = 0
# Create dictionary of antenna parameters
antennaparams = {'time': time, 'freqs': freqs, 'Vinc': Vinc, 'Vincp': Vincp, 'Iinc': Iinc, 'Iincp': Iincp,
'Vref': Vref, 'Vrefp': Vrefp, 'Iref': Iref, 'Irefp': Irefp,
'Vtotal': Vtotal, 'Vtotalp': Vtotalp, 'Itotal': Itotal, 'Itotalp': Itotalp,
's11': s11, 'zin': zin, 'yin': yin}
if tlrxnumber or rxnumber:
with np.errstate(divide='ignore'): # Ignore warning from taking a log of any zero values
s21 = 20 * np.log10(s21)
s21[np.invert(np.isfinite(s21))] = 0
antennaparams['s21'] = s21
return antennaparams
def mpl_plot(filename, time, freqs, Vinc, Vincp, Iinc, Iincp, Vref, Vrefp, Iref, Irefp, Vtotal, Vtotalp, Itotal, Itotalp, s11, zin, yin, s21=None):
"""Plots antenna parameters - incident, reflected and total volatges and currents; s11, (s21) and input impedance.
Args:
filename (string): Filename (including path) of output file.
time (array): Simulation time.
freq (array): Frequencies for FFTs.
Vinc, Vincp, Iinc, Iincp (array): Time and frequency domain representations of incident voltage and current.
Vref, Vrefp, Iref, Irefp (array): Time and frequency domain representations of reflected voltage and current.
Vtotal, Vtotalp, Itotal, Itotalp (array): Time and frequency domain representations of total voltage and current.
s11, s21 (array): s11 and, optionally, s21 parameters.
zin, yin (array): Input impedance and input admittance parameters.
Returns:
plt (object): matplotlib plot object.
"""
# Set plotting range
pltrangemin = 1
# To a certain drop from maximum power
pltrangemax = np.where((np.amax(Vincp[1::]) - Vincp[1::]) > 60)[0][0] + 1
# To a maximum frequency
# pltrangemax = np.where(freqs > 6e9)[0][0]
pltrange = np.s_[pltrangemin:pltrangemax]
# Print some useful values from s11, and input impedance
s11minfreq = np.where(s11[pltrange] == np.amin(s11[pltrange]))[0][0]
print('s11 minimum: {:g} dB at {:g} Hz'.format(np.amin(s11[pltrange]), freqs[s11minfreq + pltrangemin]))
print('At {:g} Hz...'.format(freqs[s11minfreq + pltrangemin]))
print('Input impedance: {:.1f}{:+.1f}j Ohms'.format(np.abs(zin[s11minfreq + pltrangemin]), zin[s11minfreq + pltrangemin].imag))
# print('Input admittance (mag): {:g} S'.format(np.abs(yin[s11minfreq + pltrangemin])))
# print('Input admittance (phase): {:.1f} deg'.format(np.angle(yin[s11minfreq + pltrangemin], deg=True)))
# Figure 1
# Plot incident voltage
fig1, ax = plt.subplots(num='Transmitter transmission line parameters', figsize=(20, 12), facecolor='w', edgecolor='w')
gs1 = gridspec.GridSpec(4, 2, hspace=0.7)
ax = plt.subplot(gs1[0, 0])
ax.plot(time, Vinc, 'r', lw=2, label='Vinc')
ax.set_title('Incident voltage')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Voltage [V]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of incident voltage
ax = plt.subplot(gs1[0, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Vincp[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
ax.plot(freqs[pltrange], Vincp[pltrange], 'r', lw=2)
ax.set_title('Incident voltage')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot incident current
ax = plt.subplot(gs1[1, 0])
ax.plot(time, Iinc, 'b', lw=2, label='Vinc')
ax.set_title('Incident current')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Current [A]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of incident current
ax = plt.subplot(gs1[1, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Iincp[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'b')
plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
ax.plot(freqs[pltrange], Iincp[pltrange], 'b', lw=2)
ax.set_title('Incident current')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot total voltage
ax = plt.subplot(gs1[2, 0])
ax.plot(time, Vtotal, 'r', lw=2, label='Vinc')
ax.set_title('Total (incident + reflected) voltage')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Voltage [V]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of total voltage
ax = plt.subplot(gs1[2, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Vtotalp[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
ax.plot(freqs[pltrange], Vtotalp[pltrange], 'r', lw=2)
ax.set_title('Total (incident + reflected) voltage')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot total current
ax = plt.subplot(gs1[3, 0])
ax.plot(time, Itotal, 'b', lw=2, label='Vinc')
ax.set_title('Total (incident + reflected) current')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Current [A]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of total current
ax = plt.subplot(gs1[3, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Itotalp[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'b')
plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
ax.plot(freqs[pltrange], Itotalp[pltrange], 'b', lw=2)
ax.set_title('Total (incident + reflected) current')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot reflected (reflected) voltage
# ax = plt.subplot(gs1[4, 0])
# ax.plot(time, Vref, 'r', lw=2, label='Vref')
# ax.set_title('Reflected voltage')
# ax.set_xlabel('Time [s]')
# ax.set_ylabel('Voltage [V]')
# ax.set_xlim([0, np.amax(time)])
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of reflected voltage
# ax = plt.subplot(gs1[4, 1])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], Vrefp[pltrange], '-.', use_line_collection=True)
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'r')
# plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
# ax.plot(freqs[pltrange], Vrefp[pltrange], 'r', lw=2)
# ax.set_title('Reflected voltage')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Power [dB]')
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot reflected (reflected) current
# ax = plt.subplot(gs1[5, 0])
# ax.plot(time, Iref, 'b', lw=2, label='Iref')
# ax.set_title('Reflected current')
# ax.set_xlabel('Time [s]')
# ax.set_ylabel('Current [A]')
# ax.set_xlim([0, np.amax(time)])
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of reflected current
# ax = plt.subplot(gs1[5, 1])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], Irefp[pltrange], '-.', use_line_collection=True)
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'b')
# plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
# ax.plot(freqs[pltrange], Irefp[pltrange], 'b', lw=2)
# ax.set_title('Reflected current')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Power [dB]')
# ax.grid(which='both', axis='both', linestyle='-.')
# Figure 2
# Plot frequency spectra of s11
fig2, ax = plt.subplots(num='Antenna parameters', figsize=(20, 12), facecolor='w', edgecolor='w')
gs2 = gridspec.GridSpec(2, 2, hspace=0.3)
ax = plt.subplot(gs2[0, 0])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], s11[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], s11[pltrange], 'g', lw=2)
ax.set_title('s11')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
# ax.set_xlim([0, 5e9])
# ax.set_ylim([-25, 0])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of s21
if s21 is not None:
ax = plt.subplot(gs2[0, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], s21[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], s21[pltrange], 'g', lw=2)
ax.set_title('s21')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([-25, 50])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot input resistance (real part of impedance)
ax = plt.subplot(gs2[1, 0])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], zin[pltrange].real, '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], zin[pltrange].real, 'g', lw=2)
ax.set_title('Input impedance (resistive)')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Resistance [Ohms]')
# ax.set_xlim([0.88e9, 1.02e9])
ax.set_ylim(bottom=0)
# ax.set_ylim([0, 300])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot input reactance (imaginery part of impedance)
ax = plt.subplot(gs2[1, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], zin[pltrange].imag, '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], zin[pltrange].imag, 'g', lw=2)
ax.set_title('Input impedance (reactive)')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Reactance [Ohms]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([-300, 300])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot input admittance (magnitude)
# ax = plt.subplot(gs2[2, 0])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], np.abs(yin[pltrange]), '-.', use_line_collection=True)
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'g')
# plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
# ax.plot(freqs[pltrange], np.abs(yin[pltrange]), 'g', lw=2)
# ax.set_title('Input admittance (magnitude)')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Admittance [Siemens]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([0, 0.035])
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot input admittance (phase)
# ax = plt.subplot(gs2[2, 1])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], np.angle(yin[pltrange], deg=True), '-.', use_line_collection=True)
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'g')
# plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
# ax.plot(freqs[pltrange], np.angle(yin[pltrange], deg=True), 'g', lw=2)
# ax.set_title('Input admittance (phase)')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Phase [degrees]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([-40, 100])
# ax.grid(which='both', axis='both', linestyle='-.')
# Save a PDF/PNG of the figure
# fig1.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_tl_params.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
# fig2.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_ant_params.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
# fig1.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_tl_params.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
# fig2.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_ant_params.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
return plt
if __name__ == "__main__":
# Parse command line arguments
parser = argparse.ArgumentParser(description='Plots antenna parameters (s11, s21 parameters and input impedance) from an output file containing a transmission line source.', usage='cd gprMax; python -m tools.plot_antenna_params outputfile')
parser.add_argument('outputfile', help='name of output file including path')
parser.add_argument('--tltx-num', default=1, type=int, help='transmitter antenna - transmission line number')
parser.add_argument('--tlrx-num', type=int, help='receiver antenna - transmission line number')
parser.add_argument('--rx-num', type=int, help='receiver antenna - output number')
parser.add_argument('--rx-component', type=str, help='receiver antenna - output electric field component', choices=['Ex', 'Ey', 'Ez'])
args = parser.parse_args()
antennaparams = calculate_antenna_params(args.outputfile, args.tltx_num, args.tlrx_num, args.rx_num, args.rx_component)
plthandle = mpl_plot(args.outputfile, **antennaparams)
plthandle.show()
# Copyright (C) 2015-2023: The University of Edinburgh
# Authors: Craig Warren and Antonis Giannopoulos
#
# This file is part of gprMax.
#
# gprMax is free software: you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation, either version 3 of the License, or
# (at your option) any later version.
#
# gprMax is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
#
# You should have received a copy of the GNU General Public License
# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
import argparse
import os
import sys
import h5py
import numpy as np
import matplotlib.pyplot as plt
import matplotlib.gridspec as gridspec
from gprMax.exceptions import CmdInputError
def calculate_antenna_params(filename, tltxnumber=1, tlrxnumber=None, rxnumber=None, rxcomponent=None):
"""Calculates antenna parameters - incident, reflected and total volatges and currents; s11, (s21) and input impedance.
Args:
filename (string): Filename (including path) of output file.
tltxnumber (int): Transmitter antenna - transmission line number
tlrxnumber (int): Receiver antenna - transmission line number
rxnumber (int): Receiver antenna - output number
rxcomponent (str): Receiver antenna - output electric field component
Returns:
antennaparams (dict): Antenna parameters.
"""
# Open output file and read some attributes
f = h5py.File(filename, 'r')
dxdydz = f.attrs['dx_dy_dz']
dt = f.attrs['dt']
iterations = f.attrs['Iterations']
# Calculate time array and frequency bin spacing
time = np.linspace(0, (iterations - 1) * dt, num=iterations)
df = 1 / np.amax(time)
print('Time window: {:g} s ({} iterations)'.format(np.amax(time), iterations))
print('Time step: {:g} s'.format(dt))
print('Frequency bin spacing: {:g} Hz'.format(df))
# Read/calculate voltages and currents from transmitter antenna
tltxpath = '/tls/tl' + str(tltxnumber) + '/'
# Incident voltages/currents
Vinc = f[tltxpath + 'Vinc'][:]
Iinc = f[tltxpath + 'Iinc'][:]
# Total (incident + reflected) voltages/currents
Vtotal = f[tltxpath + 'Vtotal'][:]
Itotal = f[tltxpath + 'Itotal'][:]
# Reflected voltages/currents
Vref = Vtotal - Vinc
Iref = Itotal - Iinc
# If a receiver antenna is used (with a transmission line or receiver), get received voltage for s21
if tlrxnumber:
tlrxpath = '/tls/tl' + str(tlrxnumber) + '/'
Vrec = f[tlrxpath + 'Vtotal'][:]
elif rxnumber:
rxpath = '/rxs/rx' + str(rxnumber) + '/'
availableoutputs = list(f[rxpath].keys())
if rxcomponent not in availableoutputs:
raise CmdInputError('{} output requested, but the available output for receiver {} is {}'.format(rxcomponent, rxnumber, ', '.join(availableoutputs)))
rxpath += rxcomponent
# Received voltage
if rxcomponent == 'Ex':
Vrec = f[rxpath][:] * -1 * dxdydz[0]
elif rxcomponent == 'Ey':
Vrec = f[rxpath][:] * -1 * dxdydz[1]
elif rxcomponent == 'Ez':
Vrec = f[rxpath][:] * -1 * dxdydz[2]
f.close()
# Frequency bins
freqs = np.fft.fftfreq(Vinc.size, d=dt)
# Delay correction - current lags voltage, so delay voltage to match current timestep
delaycorrection = np.exp(1j * 2 * np.pi * freqs * (dt / 2))
# Calculate s11 and (optionally) s21
with np.errstate(divide='ignore'):
s11 = np.abs(np.fft.fft(Vref) / np.fft.fft(Vinc))
if tlrxnumber or rxnumber:
with np.errstate(divide='ignore'):
s21 = np.abs(np.fft.fft(Vrec) / np.fft.fft(Vinc))
# Calculate input impedance
with np.errstate(divide='ignore'):
zin = (np.fft.fft(Vtotal) * delaycorrection) / np.fft.fft(Itotal)
# Calculate input admittance
with np.errstate(divide='ignore'):
yin = np.fft.fft(Itotal) / (np.fft.fft(Vtotal) * delaycorrection)
# Convert to decibels (ignore warning from taking a log of any zero values)
with np.errstate(divide='ignore'):
Vincp = 20 * np.log10(np.abs((np.fft.fft(Vinc) * delaycorrection)))
Iincp = 20 * np.log10(np.abs(np.fft.fft(Iinc)))
Vrefp = 20 * np.log10(np.abs((np.fft.fft(Vref) * delaycorrection)))
Irefp = 20 * np.log10(np.abs(np.fft.fft(Iref)))
Vtotalp = 20 * np.log10(np.abs((np.fft.fft(Vtotal) * delaycorrection)))
Itotalp = 20 * np.log10(np.abs(np.fft.fft(Itotal)))
s11 = 20 * np.log10(s11)
# Replace any NaNs or Infs from zero division
Vincp[np.invert(np.isfinite(Vincp))] = 0
Iincp[np.invert(np.isfinite(Iincp))] = 0
Vrefp[np.invert(np.isfinite(Vrefp))] = 0
Irefp[np.invert(np.isfinite(Irefp))] = 0
Vtotalp[np.invert(np.isfinite(Vtotalp))] = 0
Itotalp[np.invert(np.isfinite(Itotalp))] = 0
s11[np.invert(np.isfinite(s11))] = 0
# Create dictionary of antenna parameters
antennaparams = {'time': time, 'freqs': freqs, 'Vinc': Vinc, 'Vincp': Vincp, 'Iinc': Iinc, 'Iincp': Iincp,
'Vref': Vref, 'Vrefp': Vrefp, 'Iref': Iref, 'Irefp': Irefp,
'Vtotal': Vtotal, 'Vtotalp': Vtotalp, 'Itotal': Itotal, 'Itotalp': Itotalp,
's11': s11, 'zin': zin, 'yin': yin}
if tlrxnumber or rxnumber:
with np.errstate(divide='ignore'): # Ignore warning from taking a log of any zero values
s21 = 20 * np.log10(s21)
s21[np.invert(np.isfinite(s21))] = 0
antennaparams['s21'] = s21
return antennaparams
def mpl_plot(filename, time, freqs, Vinc, Vincp, Iinc, Iincp, Vref, Vrefp, Iref, Irefp, Vtotal, Vtotalp, Itotal, Itotalp, s11, zin, yin, s21=None):
"""Plots antenna parameters - incident, reflected and total volatges and currents; s11, (s21) and input impedance.
Args:
filename (string): Filename (including path) of output file.
time (array): Simulation time.
freq (array): Frequencies for FFTs.
Vinc, Vincp, Iinc, Iincp (array): Time and frequency domain representations of incident voltage and current.
Vref, Vrefp, Iref, Irefp (array): Time and frequency domain representations of reflected voltage and current.
Vtotal, Vtotalp, Itotal, Itotalp (array): Time and frequency domain representations of total voltage and current.
s11, s21 (array): s11 and, optionally, s21 parameters.
zin, yin (array): Input impedance and input admittance parameters.
Returns:
plt (object): matplotlib plot object.
"""
# Set plotting range
pltrangemin = 1
# To a certain drop from maximum power
pltrangemax = np.where((np.amax(Vincp[1::]) - Vincp[1::]) > 60)[0][0] + 1
# To a maximum frequency
# pltrangemax = np.where(freqs > 6e9)[0][0]
pltrange = np.s_[pltrangemin:pltrangemax]
# Print some useful values from s11, and input impedance
s11minfreq = np.where(s11[pltrange] == np.amin(s11[pltrange]))[0][0]
print('s11 minimum: {:g} dB at {:g} Hz'.format(np.amin(s11[pltrange]), freqs[s11minfreq + pltrangemin]))
print('At {:g} Hz...'.format(freqs[s11minfreq + pltrangemin]))
print('Input impedance: {:.1f}{:+.1f}j Ohms'.format(np.abs(zin[s11minfreq + pltrangemin]), zin[s11minfreq + pltrangemin].imag))
# print('Input admittance (mag): {:g} S'.format(np.abs(yin[s11minfreq + pltrangemin])))
# print('Input admittance (phase): {:.1f} deg'.format(np.angle(yin[s11minfreq + pltrangemin], deg=True)))
# Figure 1
# Plot incident voltage
fig1, ax = plt.subplots(num='Transmitter transmission line parameters', figsize=(20, 12), facecolor='w', edgecolor='w')
gs1 = gridspec.GridSpec(4, 2, hspace=0.7)
ax = plt.subplot(gs1[0, 0])
ax.plot(time, Vinc, 'r', lw=2, label='Vinc')
ax.set_title('Incident voltage')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Voltage [V]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of incident voltage
ax = plt.subplot(gs1[0, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Vincp[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
ax.plot(freqs[pltrange], Vincp[pltrange], 'r', lw=2)
ax.set_title('Incident voltage')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot incident current
ax = plt.subplot(gs1[1, 0])
ax.plot(time, Iinc, 'b', lw=2, label='Vinc')
ax.set_title('Incident current')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Current [A]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of incident current
ax = plt.subplot(gs1[1, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Iincp[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'b')
plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
ax.plot(freqs[pltrange], Iincp[pltrange], 'b', lw=2)
ax.set_title('Incident current')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot total voltage
ax = plt.subplot(gs1[2, 0])
ax.plot(time, Vtotal, 'r', lw=2, label='Vinc')
ax.set_title('Total (incident + reflected) voltage')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Voltage [V]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of total voltage
ax = plt.subplot(gs1[2, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Vtotalp[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
ax.plot(freqs[pltrange], Vtotalp[pltrange], 'r', lw=2)
ax.set_title('Total (incident + reflected) voltage')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot total current
ax = plt.subplot(gs1[3, 0])
ax.plot(time, Itotal, 'b', lw=2, label='Vinc')
ax.set_title('Total (incident + reflected) current')
ax.set_xlabel('Time [s]')
ax.set_ylabel('Current [A]')
ax.set_xlim([0, np.amax(time)])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of total current
ax = plt.subplot(gs1[3, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], Itotalp[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'b')
plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
ax.plot(freqs[pltrange], Itotalp[pltrange], 'b', lw=2)
ax.set_title('Total (incident + reflected) current')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
ax.grid(which='both', axis='both', linestyle='-.')
# Plot reflected (reflected) voltage
# ax = plt.subplot(gs1[4, 0])
# ax.plot(time, Vref, 'r', lw=2, label='Vref')
# ax.set_title('Reflected voltage')
# ax.set_xlabel('Time [s]')
# ax.set_ylabel('Voltage [V]')
# ax.set_xlim([0, np.amax(time)])
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of reflected voltage
# ax = plt.subplot(gs1[4, 1])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], Vrefp[pltrange], '-.')
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'r')
# plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
# ax.plot(freqs[pltrange], Vrefp[pltrange], 'r', lw=2)
# ax.set_title('Reflected voltage')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Power [dB]')
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot reflected (reflected) current
# ax = plt.subplot(gs1[5, 0])
# ax.plot(time, Iref, 'b', lw=2, label='Iref')
# ax.set_title('Reflected current')
# ax.set_xlabel('Time [s]')
# ax.set_ylabel('Current [A]')
# ax.set_xlim([0, np.amax(time)])
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of reflected current
# ax = plt.subplot(gs1[5, 1])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], Irefp[pltrange], '-.')
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'b')
# plt.setp(markerline, 'markerfacecolor', 'b', 'markeredgecolor', 'b')
# ax.plot(freqs[pltrange], Irefp[pltrange], 'b', lw=2)
# ax.set_title('Reflected current')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Power [dB]')
# ax.grid(which='both', axis='both', linestyle='-.')
# Figure 2
# Plot frequency spectra of s11
fig2, ax = plt.subplots(num='Antenna parameters', figsize=(20, 12), facecolor='w', edgecolor='w')
gs2 = gridspec.GridSpec(2, 2, hspace=0.3)
ax = plt.subplot(gs2[0, 0])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], s11[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], s11[pltrange], 'g', lw=2)
ax.set_title('s11')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
# ax.set_xlim([0, 5e9])
# ax.set_ylim([-25, 0])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot frequency spectra of s21
if s21 is not None:
ax = plt.subplot(gs2[0, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], s21[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], s21[pltrange], 'g', lw=2)
ax.set_title('s21')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Power [dB]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([-25, 50])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot input resistance (real part of impedance)
ax = plt.subplot(gs2[1, 0])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], zin[pltrange].real, '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], zin[pltrange].real, 'g', lw=2)
ax.set_title('Input impedance (resistive)')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Resistance [Ohms]')
# ax.set_xlim([0.88e9, 1.02e9])
ax.set_ylim(bottom=0)
# ax.set_ylim([0, 300])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot input reactance (imaginery part of impedance)
ax = plt.subplot(gs2[1, 1])
markerline, stemlines, baseline = ax.stem(freqs[pltrange], zin[pltrange].imag, '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'g')
plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
ax.plot(freqs[pltrange], zin[pltrange].imag, 'g', lw=2)
ax.set_title('Input impedance (reactive)')
ax.set_xlabel('Frequency [Hz]')
ax.set_ylabel('Reactance [Ohms]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([-300, 300])
ax.grid(which='both', axis='both', linestyle='-.')
# Plot input admittance (magnitude)
# ax = plt.subplot(gs2[2, 0])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], np.abs(yin[pltrange]), '-.')
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'g')
# plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
# ax.plot(freqs[pltrange], np.abs(yin[pltrange]), 'g', lw=2)
# ax.set_title('Input admittance (magnitude)')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Admittance [Siemens]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([0, 0.035])
# ax.grid(which='both', axis='both', linestyle='-.')
# Plot input admittance (phase)
# ax = plt.subplot(gs2[2, 1])
# markerline, stemlines, baseline = ax.stem(freqs[pltrange], np.angle(yin[pltrange], deg=True), '-.')
# plt.setp(baseline, 'linewidth', 0)
# plt.setp(stemlines, 'color', 'g')
# plt.setp(markerline, 'markerfacecolor', 'g', 'markeredgecolor', 'g')
# ax.plot(freqs[pltrange], np.angle(yin[pltrange], deg=True), 'g', lw=2)
# ax.set_title('Input admittance (phase)')
# ax.set_xlabel('Frequency [Hz]')
# ax.set_ylabel('Phase [degrees]')
# ax.set_xlim([0.88e9, 1.02e9])
# ax.set_ylim([-40, 100])
# ax.grid(which='both', axis='both', linestyle='-.')
# Save a PDF/PNG of the figure
# fig1.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_tl_params.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
# fig2.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_ant_params.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
# fig1.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_tl_params.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
# fig2.savefig(os.path.splitext(os.path.abspath(filename))[0] + '_ant_params.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
return plt
if __name__ == "__main__":
# Parse command line arguments
parser = argparse.ArgumentParser(description='Plots antenna parameters (s11, s21 parameters and input impedance) from an output file containing a transmission line source.', usage='cd gprMax; python -m tools.plot_antenna_params outputfile')
parser.add_argument('outputfile', help='name of output file including path')
parser.add_argument('--tltx-num', default=1, type=int, help='transmitter antenna - transmission line number')
parser.add_argument('--tlrx-num', type=int, help='receiver antenna - transmission line number')
parser.add_argument('--rx-num', type=int, help='receiver antenna - output number')
parser.add_argument('--rx-component', type=str, help='receiver antenna - output electric field component', choices=['Ex', 'Ey', 'Ez'])
args = parser.parse_args()
antennaparams = calculate_antenna_params(args.outputfile, args.tltx_num, args.tlrx_num, args.rx_num, args.rx_component)
plthandle = mpl_plot(args.outputfile, **antennaparams)
plthandle.show()

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@@ -1,173 +1,173 @@
# Copyright (C) 2015-2023: The University of Edinburgh
# Authors: Craig Warren and Antonis Giannopoulos
#
# This file is part of gprMax.
#
# gprMax is free software: you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation, either version 3 of the License, or
# (at your option) any later version.
#
# gprMax is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
#
# You should have received a copy of the GNU General Public License
# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
import argparse
import os
import sys
import numpy as np
import matplotlib.pyplot as plt
from gprMax.exceptions import CmdInputError
from gprMax.utilities import fft_power
from gprMax.utilities import round_value
from gprMax.waveforms import Waveform
def check_timewindow(timewindow, dt):
"""Checks and sets time window and number of iterations.
Args:
timewindow (float): Time window.
dt (float): Time discretisation.
Returns:
timewindow (float): Time window.
iterations (int): Number of interations.
"""
# Time window could be a string, float or int, so convert to string then check
timewindow = str(timewindow)
try:
timewindow = int(timewindow)
iterations = timewindow
timewindow = (timewindow - 1) * dt
except:
timewindow = float(timewindow)
if timewindow > 0:
iterations = round_value((timewindow / dt)) + 1
else:
raise CmdInputError('Time window must have a value greater than zero')
return timewindow, iterations
def mpl_plot(w, timewindow, dt, iterations, fft=False):
"""Plots waveform and prints useful information about its properties.
Args:
w (class): Waveform class instance.
timewindow (float): Time window.
dt (float): Time discretisation.
iterations (int): Number of iterations.
fft (boolean): Plot FFT switch.
Returns:
plt (object): matplotlib plot object.
"""
time = np.linspace(0, (iterations - 1) * dt, num=iterations)
waveform = np.zeros(len(time))
timeiter = np.nditer(time, flags=['c_index'])
while not timeiter.finished:
waveform[timeiter.index] = w.calculate_value(timeiter[0], dt)
timeiter.iternext()
print('Waveform characteristics...')
print('Type: {}'.format(w.type))
print('Maximum (absolute) amplitude: {:g}'.format(np.max(np.abs(waveform))))
if w.freq and not w.type == 'gaussian':
print('Centre frequency: {:g} Hz'.format(w.freq))
if w.type == 'gaussian' or w.type == 'gaussiandot' or w.type == 'gaussiandotnorm' or w.type == 'gaussianprime' or w.type == 'gaussiandoubleprime':
delay = 1 / w.freq
print('Time to centre of pulse: {:g} s'.format(delay))
elif w.type == 'gaussiandotdot' or w.type == 'gaussiandotdotnorm' or w.type == 'ricker':
delay = np.sqrt(2) / w.freq
print('Time to centre of pulse: {:g} s'.format(delay))
print('Time window: {:g} s ({} iterations)'.format(timewindow, iterations))
print('Time step: {:g} s'.format(dt))
if fft:
# FFT
freqs, power = fft_power(waveform, dt)
# Set plotting range to 4 times frequency at max power of waveform or
# 4 times the centre frequency
freqmaxpower = np.where(np.isclose(power, 0))[0][0]
if freqs[freqmaxpower] > w.freq:
pltrange = np.where(freqs > 4 * freqs[freqmaxpower])[0][0]
else:
pltrange = np.where(freqs > 4 * w.freq)[0][0]
pltrange = np.s_[0:pltrange]
fig, (ax1, ax2) = plt.subplots(nrows=1, ncols=2, num=w.type, figsize=(20, 10), facecolor='w', edgecolor='w')
# Plot waveform
ax1.plot(time, waveform, 'r', lw=2)
ax1.set_xlabel('Time [s]')
ax1.set_ylabel('Amplitude')
# Plot frequency spectra
markerline, stemlines, baseline = ax2.stem(freqs[pltrange], power[pltrange], '-.', use_line_collection=True)
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
ax2.plot(freqs[pltrange], power[pltrange], 'r', lw=2)
ax2.set_xlabel('Frequency [Hz]')
ax2.set_ylabel('Power [dB]')
else:
fig, ax1 = plt.subplots(num=w.type, figsize=(20, 10), facecolor='w', edgecolor='w')
# Plot waveform
ax1.plot(time, waveform, 'r', lw=2)
ax1.set_xlabel('Time [s]')
ax1.set_ylabel('Amplitude')
[ax.grid(which='both', axis='both', linestyle='-.') for ax in fig.axes] # Turn on grid
# Save a PDF/PNG of the figure
# fig.savefig(os.path.dirname(os.path.abspath(__file__)) + os.sep + w.type + '.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
# fig.savefig(os.path.dirname(os.path.abspath(__file__)) + os.sep + w.type + '.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
return plt
if __name__ == "__main__":
# Parse command line arguments
parser = argparse.ArgumentParser(description='Plot built-in waveforms that can be used for sources.', usage='cd gprMax; python -m tools.plot_source_wave type amp freq timewindow dt')
parser.add_argument('type', help='type of waveform', choices=Waveform.types)
parser.add_argument('amp', type=float, help='amplitude of waveform')
parser.add_argument('freq', type=float, help='centre frequency of waveform')
parser.add_argument('timewindow', help='time window to view waveform')
parser.add_argument('dt', type=float, help='time step to view waveform')
parser.add_argument('-fft', action='store_true', help='plot FFT of waveform', default=False)
args = parser.parse_args()
# Check waveform parameters
if args.type.lower() not in Waveform.types:
raise CmdInputError('The waveform must have one of the following types {}'.format(', '.join(Waveform.types)))
if args.freq <= 0:
raise CmdInputError('The waveform requires an excitation frequency value of greater than zero')
# Create waveform instance
w = Waveform()
w.type = args.type
w.amp = args.amp
w.freq = args.freq
timewindow, iterations = check_timewindow(args.timewindow, args.dt)
plthandle = mpl_plot(w, timewindow, args.dt, iterations, args.fft)
plthandle.show()
# Copyright (C) 2015-2023: The University of Edinburgh
# Authors: Craig Warren and Antonis Giannopoulos
#
# This file is part of gprMax.
#
# gprMax is free software: you can redistribute it and/or modify
# it under the terms of the GNU General Public License as published by
# the Free Software Foundation, either version 3 of the License, or
# (at your option) any later version.
#
# gprMax is distributed in the hope that it will be useful,
# but WITHOUT ANY WARRANTY; without even the implied warranty of
# MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
# GNU General Public License for more details.
#
# You should have received a copy of the GNU General Public License
# along with gprMax. If not, see <http://www.gnu.org/licenses/>.
import argparse
import os
import sys
import numpy as np
import matplotlib.pyplot as plt
from gprMax.exceptions import CmdInputError
from gprMax.utilities import fft_power
from gprMax.utilities import round_value
from gprMax.waveforms import Waveform
def check_timewindow(timewindow, dt):
"""Checks and sets time window and number of iterations.
Args:
timewindow (float): Time window.
dt (float): Time discretisation.
Returns:
timewindow (float): Time window.
iterations (int): Number of interations.
"""
# Time window could be a string, float or int, so convert to string then check
timewindow = str(timewindow)
try:
timewindow = int(timewindow)
iterations = timewindow
timewindow = (timewindow - 1) * dt
except:
timewindow = float(timewindow)
if timewindow > 0:
iterations = round_value((timewindow / dt)) + 1
else:
raise CmdInputError('Time window must have a value greater than zero')
return timewindow, iterations
def mpl_plot(w, timewindow, dt, iterations, fft=False):
"""Plots waveform and prints useful information about its properties.
Args:
w (class): Waveform class instance.
timewindow (float): Time window.
dt (float): Time discretisation.
iterations (int): Number of iterations.
fft (boolean): Plot FFT switch.
Returns:
plt (object): matplotlib plot object.
"""
time = np.linspace(0, (iterations - 1) * dt, num=iterations)
waveform = np.zeros(len(time))
timeiter = np.nditer(time, flags=['c_index'])
while not timeiter.finished:
waveform[timeiter.index] = w.calculate_value(timeiter[0], dt)
timeiter.iternext()
print('Waveform characteristics...')
print('Type: {}'.format(w.type))
print('Maximum (absolute) amplitude: {:g}'.format(np.max(np.abs(waveform))))
if w.freq and not w.type == 'gaussian':
print('Centre frequency: {:g} Hz'.format(w.freq))
if w.type == 'gaussian' or w.type == 'gaussiandot' or w.type == 'gaussiandotnorm' or w.type == 'gaussianprime' or w.type == 'gaussiandoubleprime':
delay = 1 / w.freq
print('Time to centre of pulse: {:g} s'.format(delay))
elif w.type == 'gaussiandotdot' or w.type == 'gaussiandotdotnorm' or w.type == 'ricker':
delay = np.sqrt(2) / w.freq
print('Time to centre of pulse: {:g} s'.format(delay))
print('Time window: {:g} s ({} iterations)'.format(timewindow, iterations))
print('Time step: {:g} s'.format(dt))
if fft:
# FFT
freqs, power = fft_power(waveform, dt)
# Set plotting range to 4 times frequency at max power of waveform or
# 4 times the centre frequency
freqmaxpower = np.where(np.isclose(power, 0))[0][0]
if freqs[freqmaxpower] > w.freq:
pltrange = np.where(freqs > 4 * freqs[freqmaxpower])[0][0]
else:
pltrange = np.where(freqs > 4 * w.freq)[0][0]
pltrange = np.s_[0:pltrange]
fig, (ax1, ax2) = plt.subplots(nrows=1, ncols=2, num=w.type, figsize=(20, 10), facecolor='w', edgecolor='w')
# Plot waveform
ax1.plot(time, waveform, 'r', lw=2)
ax1.set_xlabel('Time [s]')
ax1.set_ylabel('Amplitude')
# Plot frequency spectra
markerline, stemlines, baseline = ax2.stem(freqs[pltrange], power[pltrange], '-.')
plt.setp(baseline, 'linewidth', 0)
plt.setp(stemlines, 'color', 'r')
plt.setp(markerline, 'markerfacecolor', 'r', 'markeredgecolor', 'r')
ax2.plot(freqs[pltrange], power[pltrange], 'r', lw=2)
ax2.set_xlabel('Frequency [Hz]')
ax2.set_ylabel('Power [dB]')
else:
fig, ax1 = plt.subplots(num=w.type, figsize=(20, 10), facecolor='w', edgecolor='w')
# Plot waveform
ax1.plot(time, waveform, 'r', lw=2)
ax1.set_xlabel('Time [s]')
ax1.set_ylabel('Amplitude')
[ax.grid(which='both', axis='both', linestyle='-.') for ax in fig.axes] # Turn on grid
# Save a PDF/PNG of the figure
# fig.savefig(os.path.dirname(os.path.abspath(__file__)) + os.sep + w.type + '.pdf', dpi=None, format='pdf', bbox_inches='tight', pad_inches=0.1)
# fig.savefig(os.path.dirname(os.path.abspath(__file__)) + os.sep + w.type + '.png', dpi=150, format='png', bbox_inches='tight', pad_inches=0.1)
return plt
if __name__ == "__main__":
# Parse command line arguments
parser = argparse.ArgumentParser(description='Plot built-in waveforms that can be used for sources.', usage='cd gprMax; python -m tools.plot_source_wave type amp freq timewindow dt')
parser.add_argument('type', help='type of waveform', choices=Waveform.types)
parser.add_argument('amp', type=float, help='amplitude of waveform')
parser.add_argument('freq', type=float, help='centre frequency of waveform')
parser.add_argument('timewindow', help='time window to view waveform')
parser.add_argument('dt', type=float, help='time step to view waveform')
parser.add_argument('-fft', action='store_true', help='plot FFT of waveform', default=False)
args = parser.parse_args()
# Check waveform parameters
if args.type.lower() not in Waveform.types:
raise CmdInputError('The waveform must have one of the following types {}'.format(', '.join(Waveform.types)))
if args.freq <= 0:
raise CmdInputError('The waveform requires an excitation frequency value of greater than zero')
# Create waveform instance
w = Waveform()
w.type = args.type
w.amp = args.amp
w.freq = args.freq
timewindow, iterations = check_timewindow(args.timewindow, args.dt)
plthandle = mpl_plot(w, timewindow, args.dt, iterations, args.fft)
plthandle.show()