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Re-structuring package layout

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Craig Warren
2022-11-09 09:29:23 +00:00
父节点 50d17f33ef
当前提交 16df30968e
共有 269 个文件被更改，包括 14 次插入 和 261 次删除
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143
testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate.py 可执行文件
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from pathlib import Path
import gprMax
import numpy as np
# File path for output
fn = Path(__file__)
parts = fn.parts
# Discretisation
dl = 0.001
# Domain
x = 0.051
y = 0.126
z = 0.026
domain = gprMax.Domain(p1=(x, y, z))
dxdydz = gprMax.Discretisation(p1=(dl, dl, dl))
time_window = gprMax.TimeWindow(iterations=2100)
tssf = gprMax.TimeStepStabilityFactor(f=0.99)
waveform = gprMax.Waveform(wave_type='gaussiandotnorm', amp=1, freq=9.42e9, id='mypulse')
hertzian_dipole = gprMax.HertzianDipole(polarisation='z',
p1=(0.013, 0.013, 0.014),
waveform_id='mypulse')
rx = gprMax.Rx(p1=(0.038, 0.114, 0.013))
plate = gprMax.Plate(p1=(0.013, 0.013, 0.013),
p2=(0.038, 0.113, 0.013), material_id='pec')
gv1 = gprMax.GeometryView(p1=(0, 0, 0), p2=(x, y, z), dl=(dl, dl, dl),
filename=Path(*parts[:-1], parts[-1] + '_n'), output_type='n')
gv2 = gprMax.GeometryView(p1=(0, 0, 0), p2=(x, y, z), dl=(dl, dl, dl),
filename=Path(*parts[:-1], parts[-1] + '_f'), output_type='f')
pmls = {'CFS-PML': {'pml_type': gprMax.PMLFormulation(pml='HORIPML'),
# Parameters from http://dx.doi.org/10.1109/TAP.2018.2823864
'pml_cfs': [gprMax.PMLCFS(alphascalingprofile='constant',
alphascalingdirection='forward',
alphamin=0.05, alphamax=0.05,
kappascalingprofile='quartic',
kappascalingdirection='forward',
kappamin=1, kappamax=8,
sigmascalingprofile='quartic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=1.1 * ((4 + 1) / (150 * np.pi * dl)))]},
'HORIPML-1': {'pml_type': gprMax.PMLFormulation(pml='HORIPML'),
# Parameters from http://dx.doi.org/10.1109/TAP.2011.2180344
'pml_cfs': [gprMax.PMLCFS(alphascalingprofile='constant',
alphascalingdirection='forward',
alphamin=0, alphamax=0,
kappascalingprofile='quartic',
kappascalingdirection='forward',
kappamin=1, kappamax=12,
sigmascalingprofile='quartic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=0.7 * ((4 + 1) / (150 * np.pi * dl)))]},
'HORIPML-2': {'pml_type': gprMax.PMLFormulation(pml='HORIPML'),
# Parameters from http://dx.doi.org/10.1109/TAP.2018.2823864
'pml_cfs': [gprMax.PMLCFS(alphascalingprofile='constant',
alphascalingdirection='forward',
alphamin=0, alphamax=0,
kappascalingprofile='constant',
kappascalingdirection='forward',
kappamin=1, kappamax=1,
sigmascalingprofile='sextic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=0.275 / (150 * np.pi * dl)),
gprMax.PMLCFS(alphascalingprofile='sextic',
alphascalingdirection='forward',
alphamin=0.07, alphamax=0.07 + (0.275 / (150 * np.pi * dl)),
kappascalingprofile='cubic',
kappascalingdirection='forward',
kappamin=1, kappamax=8,
sigmascalingprofile='quadratic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=2.75 / (150 * np.pi * dl))]},
'MRIPML-1': {'pml_type': gprMax.PMLFormulation(pml='MRIPML'),
# Parameters from Antonis' MATLAB script (M3Dparams.m)
'pml_cfs': [gprMax.PMLCFS(alphascalingprofile='constant',
alphascalingdirection='forward',
alphamin=0.05, alphamax=0.05,
kappascalingprofile='quartic',
kappascalingdirection='forward',
kappamin=1, kappamax=8,
sigmascalingprofile='quartic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=1.1 * ((4 + 1) / (150 * np.pi * dl)))]},
'MRIPML-2': {'pml_type': gprMax.PMLFormulation(pml='MRIPML'),
# Parameters from http://dx.doi.org/10.1109/TAP.2018.2823864
'pml_cfs': [gprMax.PMLCFS(alphascalingprofile='quadratic',
alphascalingdirection='reverse',
alphamin=0, alphamax=0.15,
kappascalingprofile='quartic',
kappascalingdirection='forward',
kappamin=1, kappamax=12,
sigmascalingprofile='quartic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=0.65 * ((4 + 1) / (150 * np.pi * dl))),
gprMax.PMLCFS(alphascalingprofile='linear',
alphascalingdirection='reverse',
alphamin=0.07, alphamax=0.8,
kappascalingprofile='constant',
kappascalingdirection='forward',
kappamin=0, kappamax=0,
sigmascalingprofile='quadratic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=0.65 * ((2 + 1) / (150 * np.pi * dl)))]}
}
scenes = []
for k, v in pmls.items():
scene = gprMax.Scene()
title = gprMax.Title(name=fn.with_suffix('').name + '_' + k)
scene.add(title)
scene.add(domain)
scene.add(dxdydz)
scene.add(time_window)
scene.add(tssf)
scene.add(waveform)
scene.add(hertzian_dipole)
scene.add(rx)
# scene.add(gv1)
# scene.add(gv2)
pml_cells = gprMax.PMLCells(thickness=10)
scene.add(pml_cells)
scene.add(v['pml_type'])
for pml_cfs in v['pml_cfs']:
scene.add(pml_cfs)
scenes.append(scene)
# Run model
gprMax.run(scenes=scenes, n=len(pmls), geometry_only=False, outputfile=fn)

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testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate1.h5 普通文件
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testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate2.h5 普通文件
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testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate3.h5 普通文件
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testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate4.h5 普通文件
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testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate5.h5 普通文件
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testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate_ref.h5 普通文件
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34
testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate_ref.in 可执行文件
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#title: Standard PML of response from an elongated thin PEC plate
#domain: 0.201 0.276 0.176
#dx_dy_dz: 0.001 0.001 0.001
#time_window: 2100
#time_step_stability_factor: 0.99
################################################
## PML parameters
## CFS (alpha, kappa, sigma)
## sigma_max = (0.8 * (m + 1)) / (z0 * d * np.sqrt(er * mr))
## z0 = 376.73, d = 0.001
################################################
#pml_cells: 10
#############
## CFS PML ##
#############
#python:
import numpy as np
# Parameters from http://dx.doi.org/10.1109/TAP.2018.2823864
smax = 1.1 * ((4 + 1) / (150 * np.pi * 0.001))
print('#pml_cfs: constant forward 0.05 0.05 quartic forward 1 8 quartic forward 0 {}'.format(smax))
#end_python:
#waveform: gaussiandotnorm 1 9.42e9 mypulse
#hertzian_dipole: z 0.088 0.088 0.089 mypulse
#rx: 0.113 0.189 0.088
#plate: 0.088 0.088 0.088 0.113 0.188 0.088 pec
geometry_view: 0 0 0 0.201 0.276 0.176 0.001 0.001 0.001 pml_3D_pec_plate_ref_f f
geometry_view: 0 0 0 0.201 0.276 0.176 0.001 0.001 0.001 pml_3D_pec_plate_ref_n n

70
testing/models_pmls/pml_3D_pec_plate/pml_3D_pec_plate_ref.py 可执行文件
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from pathlib import Path
import gprMax
import numpy as np
# File path for output
fn = Path(__file__)
parts = fn.parts
# Discretisation
dl = 0.001
# Domain
x = 0.201
y = 0.276
z = 0.176
domain = gprMax.Domain(p1=(x, y, z))
dxdydz = gprMax.Discretisation(p1=(dl, dl, dl))
time_window = gprMax.TimeWindow(iterations=2100)
tssf = gprMax.TimeStepStabilityFactor(f=0.99)
waveform = gprMax.Waveform(wave_type='gaussiandotnorm', amp=1, freq=9.42e9, id='mypulse')
hertzian_dipole = gprMax.HertzianDipole(polarisation='z',
p1=(0.088, 0.088, 0.089),
waveform_id='mypulse')
rx = gprMax.Rx(p1=(0.113, 0.189, 0.088))
plate = gprMax.Plate(p1=(0.088, 0.088, 0.088),
p2=(0.113, 0.188, 0.088), material_id='pec')
gv1 = gprMax.GeometryView(p1=(0, 0, 0), p2=(x, y, z), dl=(dl, dl, dl),
filename=Path(*parts[:-1], parts[-1] + '_n'), output_type='n')
gv2 = gprMax.GeometryView(p1=(0, 0, 0), p2=(x, y, z), dl=(dl, dl, dl),
filename=Path(*parts[:-1], parts[-1] + '_f'), output_type='f')
pml_type = gprMax.PMLFormulation(pml='HORIPML')
pml_cells = gprMax.PMLCells(thickness=10)
# Parameters from http://dx.doi.org/10.1109/TAP.2018.2823864
pml_cfs = gprMax.PMLCFS(alphascalingprofile='constant',
alphascalingdirection='forward',
alphamin=0.05, alphamax=0.05,
kappascalingprofile='quartic',
kappascalingdirection='forward',
kappamin=1, kappamax=8,
sigmascalingprofile='quartic',
sigmascalingdirection='forward',
sigmamin=0,
sigmamax=1.1 * ((4 + 1) / (150 * np.pi * dl)))
scene = gprMax.Scene()
title = gprMax.Title(name=fn.with_suffix('').name + '_ref')
scene.add(title)
scene.add(domain)
scene.add(dxdydz)
scene.add(time_window)
scene.add(tssf)
scene.add(waveform)
scene.add(hertzian_dipole)
scene.add(rx)
# scene.add(gv1)
# scene.add(gv2)
scene.add(pml_cells)
scene.add(pml_type)
scene.add(pml_cfs)
# Run model
gprMax.run(scenes=[scene], geometry_only=False, outputfile=fn)