Changed to new-style classes.

Added better dispersion checking for sine, contsine, impulse and user.
Separated field array initialisation into its own method.
这个提交包含在:
Craig Warren
2016-05-06 16:28:46 +01:00
父节点 7402c20112
当前提交 e9b4f476a7

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@@ -23,7 +23,7 @@ from gprMax.constants import c, floattype, complextype
from gprMax.materials import Material
class FDTDGrid:
class FDTDGrid(object):
"""Holds attributes associated with the entire grid. A convenient way for accessing regularly used parameters."""
def __init__(self):
@@ -54,25 +54,27 @@ class FDTDGrid:
self.hertziandipoles = []
self.magneticdipoles = []
self.transmissionlines = []
self.rxs = []
self.srcstepx = 0
self.srcstepy = 0
self.srcstepz = 0
self.rxstepx = 0
self.rxstepy = 0
self.rxstepz = 0
self.rxs = []
self.snapshots = []
def initialise_std_arrays(self):
def initialise_geometry_arrays(self):
"""Initialise an array for volumetric material IDs (solid); boolean arrays for specifying whether materials can have dielectric smoothing (rigid);
an array for cell edge IDs (ID); and arrays for the electric and magnetic field components. Solid and ID arrays are initialised to free_space (one); rigid arrays
to allow dielectric smoothing (zero).
and an array for cell edge IDs (ID). Solid and ID arrays are initialised to free_space (one); rigid arrays to allow dielectric smoothing (zero).
"""
self.solid = np.ones((self.nx + 1, self.ny + 1, self.nz + 1), dtype=np.uint32)
self.rigidE = np.zeros((12, self.nx + 1, self.ny + 1, self.nz + 1), dtype=np.int8)
self.rigidH = np.zeros((6, self.nx + 1, self.ny + 1, self.nz + 1), dtype=np.int8)
self.IDlookup = {'Ex': 0, 'Ey': 1, 'Ez': 2, 'Hx': 3, 'Hy': 4, 'Hz': 5}
self.ID = np.ones((6, self.nx + 1, self.ny + 1, self.nz + 1), dtype=np.uint32)
def initialise_field_arrays(self):
"""Initialise arrays for the electric and magnetic field components."""
self.Ex = np.zeros((self.nx, self.ny + 1, self.nz + 1), dtype=floattype)
self.Ey = np.zeros((self.nx + 1, self.ny, self.nz + 1), dtype=floattype)
self.Ez = np.zeros((self.nx + 1, self.ny + 1, self.nz), dtype=floattype)
@@ -80,7 +82,7 @@ class FDTDGrid:
self.Hy = np.zeros((self.nx, self.ny + 1, self.nz), dtype=floattype)
self.Hz = np.zeros((self.nx, self.ny, self.nz + 1), dtype=floattype)
def initialise_std_updatecoeff_arrays(self):
def initialise_std_update_coeff_arrays(self):
"""Initialise arrays for storing update coefficients."""
self.updatecoeffsE = np.zeros((len(self.materials), 5), dtype=floattype)
self.updatecoeffsH = np.zeros((len(self.materials), 5), dtype=floattype)
@@ -109,21 +111,6 @@ def dispersion_check(G):
# Find maximum frequency
maxfreqs = []
for waveform in G.waveforms:
# User-defined waveform
if waveform.uservalues is not None:
waveformvalues = waveform.uservalues
# Built-in waveform
else:
time = np.linspace(0, 1, G.iterations)
time *= (G.iterations * G.dt)
waveformvalues = np.zeros(len(time))
timeiter = np.nditer(time, flags=['c_index'])
while not timeiter.finished:
waveformvalues[timeiter.index] = waveform.calculate_value(timeiter[0], G.dt)
timeiter.iternext()
if waveform.type == 'sine' or waveform.type == 'contsine':
maxfreqs.append(4 * waveform.freq)
@@ -132,6 +119,21 @@ def dispersion_check(G):
pass
else:
# User-defined waveform
if waveform.type == 'user':
waveformvalues = waveform.uservalues
# Built-in waveform
else:
time = np.linspace(0, 1, G.iterations)
time *= (G.iterations * G.dt)
waveformvalues = np.zeros(len(time))
timeiter = np.nditer(time, flags=['c_index'])
while not timeiter.finished:
waveformvalues[timeiter.index] = waveform.calculate_value(timeiter[0], G.dt)
timeiter.iternext()
# Calculate magnitude of frequency spectra of waveform
power = 20 * np.log10(np.abs(np.fft.fft(waveformvalues))**2)
freqs = np.fft.fftfreq(power.size, d=G.dt)
@@ -160,7 +162,7 @@ def dispersion_check(G):
resolution = minwavelength / resolvedsteps
else:
resolution = 0
resolution = False
return resolution