文件
gprMax/gprMax/grid/fdtd_grid.py
2024-07-15 16:25:20 +01:00

873 行
34 KiB
Python

# Copyright (C) 2015-2024: The University of Edinburgh, United Kingdom
# Authors: Craig Warren, Antonis Giannopoulos, and John Hartley
#
# 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 decimal
import itertools
import logging
import sys
from collections import OrderedDict
from typing import Any, Iterable, List, Tuple, Union
import numpy as np
from terminaltables import AsciiTable
from tqdm import tqdm
from typing_extensions import TypeVar
from gprMax import config
from gprMax.cython.pml_build import pml_average_er_mr
from gprMax.cython.yee_cell_build import build_electric_components, build_magnetic_components
from gprMax.fractals import FractalVolume
from gprMax.materials import ListMaterial, Material, PeplinskiSoil, RangeMaterial, process_materials
from gprMax.pml import CFS, PML, print_pml_info
from gprMax.receivers import Rx
from gprMax.snapshots import Snapshot
from gprMax.sources import HertzianDipole, MagneticDipole, Source, TransmissionLine, VoltageSource
from gprMax.utilities.utilities import fft_power, get_terminal_width, round_value
from gprMax.waveforms import Waveform
logger = logging.getLogger(__name__)
class FDTDGrid:
"""Holds attributes associated with entire grid. A convenient way for
accessing regularly used parameters.
"""
IDlookup = {"Ex": 0, "Ey": 1, "Ez": 2, "Hx": 3, "Hy": 4, "Hz": 5}
def __init__(self):
self.name = "main_grid"
self.mem_use = 0
self.nx = 0
self.ny = 0
self.nz = 0
self.dl = np.ones(3, dtype=float)
self.dt = 0.0
# Field Arrays
self.Ex: np.ndarray[Any, np.dtype[np.single]]
self.Ey: np.ndarray[Any, np.dtype[np.single]]
self.Ez: np.ndarray[Any, np.dtype[np.single]]
self.Hx: np.ndarray[Any, np.dtype[np.single]]
self.Hy: np.ndarray[Any, np.dtype[np.single]]
self.Hz: np.ndarray[Any, np.dtype[np.single]]
# Dispersive Arrays
self.Tx: np.ndarray[Any, np.dtype[np.single]]
self.Ty: np.ndarray[Any, np.dtype[np.single]]
self.Tz: np.ndarray[Any, np.dtype[np.single]]
# Geometry Arrays
self.solid: np.ndarray[Any, np.dtype[np.uint32]]
self.rigidE: np.ndarray[Any, np.dtype[np.int8]]
self.rigidH: np.ndarray[Any, np.dtype[np.int8]]
self.ID: np.ndarray[Any, np.dtype[np.uint32]]
# Update Coefficient Arrays
self.updatecoeffsE: np.ndarray
self.updatecoeffsH: np.ndarray
self.updatecoeffsdispersive: np.ndarray
# PML parameters - set some defaults to use if not user provided
self.pmls = {}
self.pmls["formulation"] = "HORIPML"
self.pmls["cfs"] = []
self.pmls["slabs"] = []
# Ordered dictionary required so *updating* the PMLs always follows the
# same order (the order for *building* PMLs does not matter). The order
# itself does not matter, however, if must be the same from model to
# model otherwise the numerical precision from adding the PML
# corrections will be different.
self.pmls["thickness"] = OrderedDict((key, 10) for key in PML.boundaryIDs)
# Materials used by this grid
self.materials: List[Material] = []
self.mixingmodels: List[Union[PeplinskiSoil, RangeMaterial, ListMaterial]] = []
self.fractalvolumes: List[FractalVolume] = []
# Sources and receivers contained inside this grid
self.waveforms: List[Waveform] = []
self.voltagesources: List[VoltageSource] = []
self.hertziandipoles: List[HertzianDipole] = []
self.magneticdipoles: List[MagneticDipole] = []
self.transmissionlines: List[TransmissionLine] = []
self.rxs: List[Rx] = []
self.snapshots: List[Snapshot] = []
self.averagevolumeobjects = True
@property
def dx(self) -> float:
return self.dl[0]
@dx.setter
def dx(self, value: float):
self.dl[0] = value
@property
def dy(self) -> float:
return self.dl[1]
@dy.setter
def dy(self, value: float):
self.dl[1] = value
@property
def dz(self) -> float:
return self.dl[2]
@dz.setter
def dz(self, value: float):
self.dl[2] = value
def build(self) -> None:
# Set default CFS parameter for PMLs if not user provided
if not self.pmls["cfs"]:
self.pmls["cfs"] = [CFS()]
logger.info(print_pml_info(self))
if not all(value == 0 for value in self.pmls["thickness"].values()):
self._build_pmls()
if self.averagevolumeobjects:
self._build_components()
self._tm_grid_update()
self._create_voltage_source_materials()
self.initialise_field_arrays()
self.initialise_std_update_coeff_arrays()
if config.get_model_config().materials["maxpoles"] > 0:
self.initialise_dispersive_arrays()
self.initialise_dispersive_update_coeff_array()
self._build_materials()
def _build_pmls(self) -> None:
pbar = tqdm(
total=sum(1 for value in self.pmls["thickness"].values() if value > 0),
desc=f"Building PML boundaries [{self.name}]",
ncols=get_terminal_width() - 1,
file=sys.stdout,
disable=not config.sim_config.general["progressbars"],
)
for pml_id, thickness in self.pmls["thickness"].items():
if thickness > 0:
pml = self._construct_pml(pml_id, thickness)
averageer, averagemr = self._calculate_average_pml_material_properties(pml)
logger.debug(
f"PML {pml.ID}: Average permittivity = {averageer}, Average permeability = {averagemr}"
)
pml.calculate_update_coeffs(averageer, averagemr)
self.pmls["slabs"].append(pml)
pbar.update()
pbar.close()
PmlType = TypeVar("PmlType", bound=PML)
def _construct_pml(self, pml_ID: str, thickness: int, pml_type: type[PmlType] = PML) -> PmlType:
"""Builds instances of the PML and calculates the initial parameters and
coefficients including setting profile (based on underlying material
er and mr from solid array).
Args:
G: FDTDGrid class describing a grid in a model.
pml_ID: string identifier of PML slab.
thickness: int with thickness of PML slab in cells.
"""
if pml_ID == "x0":
pml = pml_type(
self,
ID=pml_ID,
direction="xminus",
xs=0,
xf=thickness,
ys=0,
yf=self.ny,
zs=0,
zf=self.nz,
)
elif pml_ID == "xmax":
pml = pml_type(
self,
ID=pml_ID,
direction="xplus",
xs=self.nx - thickness,
xf=self.nx,
ys=0,
yf=self.ny,
zs=0,
zf=self.nz,
)
elif pml_ID == "y0":
pml = pml_type(
self,
ID=pml_ID,
direction="yminus",
xs=0,
xf=self.nx,
ys=0,
yf=thickness,
zs=0,
zf=self.nz,
)
elif pml_ID == "ymax":
pml = pml_type(
self,
ID=pml_ID,
direction="yplus",
xs=0,
xf=self.nx,
ys=self.ny - thickness,
yf=self.ny,
zs=0,
zf=self.nz,
)
elif pml_ID == "z0":
pml = pml_type(
self,
ID=pml_ID,
direction="zminus",
xs=0,
xf=self.nx,
ys=0,
yf=self.ny,
zs=0,
zf=thickness,
)
elif pml_ID == "zmax":
pml = pml_type(
self,
ID=pml_ID,
direction="zplus",
xs=0,
xf=self.nx,
ys=0,
yf=self.ny,
zs=self.nz - thickness,
zf=self.nz,
)
else:
raise ValueError(f"Unknown PML ID '{pml_ID}'")
return pml
def _calculate_average_pml_material_properties(self, pml: PML) -> Tuple[float, float]:
# Arrays to hold values of permittivity and permeability (avoids accessing
# Material class in Cython.)
ers = np.zeros(len(self.materials))
mrs = np.zeros(len(self.materials))
for i, m in enumerate(self.materials):
ers[i] = m.er
mrs[i] = m.mr
if pml.ID[0] == "x":
n1 = self.ny
n2 = self.nz
solid = self.solid[pml.xs, :, :]
elif pml.ID[0] == "y":
n1 = self.nx
n2 = self.nz
solid = self.solid[:, pml.ys, :]
elif pml.ID[0] == "z":
n1 = self.nx
n2 = self.ny
solid = self.solid[:, :, pml.zs]
else:
raise ValueError(f"Unknown PML ID '{pml.ID}'")
return pml_average_er_mr(n1, n2, config.get_model_config().ompthreads, solid, ers, mrs)
def _build_components(self) -> None:
# Build the model, i.e. set the material properties (ID) for every edge
# of every Yee cell
pbar = tqdm(
total=2,
desc=f"Building Yee cells [{self.name}]",
ncols=get_terminal_width() - 1,
file=sys.stdout,
disable=not config.sim_config.general["progressbars"],
)
build_electric_components(self.solid, self.rigidE, self.ID, self)
pbar.update()
build_magnetic_components(self.solid, self.rigidH, self.ID, self)
pbar.update()
pbar.close()
def _tm_grid_update(self) -> None:
if config.get_model_config().mode == "2D TMx":
self.tmx()
elif config.get_model_config().mode == "2D TMy":
self.tmy()
elif config.get_model_config().mode == "2D TMz":
self.tmz()
def _create_voltage_source_materials(self):
# Process any voltage sources (that have resistance) to create a new
# material at the source location
for voltagesource in self.voltagesources:
voltagesource.create_material(self)
def _build_materials(self) -> None:
# Process complete list of materials - calculate update coefficients,
# store in arrays, and build text list of materials/properties
materialsdata = process_materials(self)
# materialstable = SingleTable(materialsdata)
materialstable = AsciiTable(materialsdata)
materialstable.outer_border = False
materialstable.justify_columns[0] = "right"
logger.info("")
logger.info(f"Materials [{self.name}]:")
logger.info(f"{materialstable.table}\n")
def _update_positions(
self, items: Iterable[Union[Source, Rx]], step_size: List[int], step_number: int
) -> None:
if step_size[0] != 0 or step_size[1] != 0 or step_size[2] != 0:
for item in items:
if step_number == 0:
if (
item.xcoord + step_size[0] * config.sim_config.model_end < 0
or item.xcoord + step_size[0] * config.sim_config.model_end > self.nx
or item.ycoord + step_size[1] * config.sim_config.model_end < 0
or item.ycoord + step_size[1] * config.sim_config.model_end > self.ny
or item.zcoord + step_size[2] * config.sim_config.model_end < 0
or item.zcoord + step_size[2] * config.sim_config.model_end > self.nz
):
raise ValueError
item.xcoord = item.xcoordorigin + step_number * step_size[0]
item.ycoord = item.ycoordorigin + step_number * step_size[1]
item.zcoord = item.zcoordorigin + step_number * step_size[2]
def update_simple_source_positions(self, step_size: List[int], step: int = 0) -> None:
try:
self._update_positions(
itertools.chain(self.hertziandipoles, self.magneticdipoles), step_size, step
)
except ValueError as e:
logger.exception("Source(s) will be stepped to a position outside the domain.")
raise ValueError from e
def update_receiver_positions(self, step_size: List[int], step: int = 0) -> None:
try:
self._update_positions(self.rxs, step_size, step)
except ValueError as e:
logger.exception("Receiver(s) will be stepped to a position outside the domain.")
raise ValueError from e
def within_bounds(self, p):
if p[0] < 0 or p[0] > self.nx:
raise ValueError("x")
if p[1] < 0 or p[1] > self.ny:
raise ValueError("y")
if p[2] < 0 or p[2] > self.nz:
raise ValueError("z")
def discretise_point(self, p):
x = round_value(float(p[0]) / self.dx)
y = round_value(float(p[1]) / self.dy)
z = round_value(float(p[2]) / self.dz)
return (x, y, z)
def round_to_grid(self, p):
p = self.discretise_point(p)
p_r = (p[0] * self.dx, p[1] * self.dy, p[2] * self.dz)
return p_r
def within_pml(self, p):
if (
p[0] < self.pmls["thickness"]["x0"]
or p[0] > self.nx - self.pmls["thickness"]["xmax"]
or p[1] < self.pmls["thickness"]["y0"]
or p[1] > self.ny - self.pmls["thickness"]["ymax"]
or p[2] < self.pmls["thickness"]["z0"]
or p[2] > self.nz - self.pmls["thickness"]["zmax"]
):
return True
else:
return False
def get_waveform_by_id(self, waveform_id: str) -> Waveform:
return next(waveform for waveform in self.waveforms if waveform.ID == waveform_id)
def initialise_geometry_arrays(self):
"""Initialise an array for volumetric material IDs (solid);
boolean arrays for specifying whether materials can have dielectric
smoothing (rigid); 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, self.ny, self.nz), dtype=np.uint32)
self.rigidE = np.zeros((12, self.nx, self.ny, self.nz), dtype=np.int8)
self.rigidH = np.zeros((6, self.nx, self.ny, self.nz), dtype=np.int8)
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 + 1, self.ny + 1, self.nz + 1),
dtype=config.sim_config.dtypes["float_or_double"],
)
self.Ey = np.zeros(
(self.nx + 1, self.ny + 1, self.nz + 1),
dtype=config.sim_config.dtypes["float_or_double"],
)
self.Ez = np.zeros(
(self.nx + 1, self.ny + 1, self.nz + 1),
dtype=config.sim_config.dtypes["float_or_double"],
)
self.Hx = np.zeros(
(self.nx + 1, self.ny + 1, self.nz + 1),
dtype=config.sim_config.dtypes["float_or_double"],
)
self.Hy = np.zeros(
(self.nx + 1, self.ny + 1, self.nz + 1),
dtype=config.sim_config.dtypes["float_or_double"],
)
self.Hz = np.zeros(
(self.nx + 1, self.ny + 1, self.nz + 1),
dtype=config.sim_config.dtypes["float_or_double"],
)
def initialise_std_update_coeff_arrays(self):
"""Initialise arrays for storing update coefficients."""
self.updatecoeffsE = np.zeros(
(len(self.materials), 5), dtype=config.sim_config.dtypes["float_or_double"]
)
self.updatecoeffsH = np.zeros(
(len(self.materials), 5), dtype=config.sim_config.dtypes["float_or_double"]
)
def initialise_dispersive_arrays(self):
"""Initialise field arrays when there are dispersive materials present."""
self.Tx = np.zeros(
(
config.get_model_config().materials["maxpoles"],
self.nx + 1,
self.ny + 1,
self.nz + 1,
),
dtype=config.get_model_config().materials["dispersivedtype"],
)
self.Ty = np.zeros(
(
config.get_model_config().materials["maxpoles"],
self.nx + 1,
self.ny + 1,
self.nz + 1,
),
dtype=config.get_model_config().materials["dispersivedtype"],
)
self.Tz = np.zeros(
(
config.get_model_config().materials["maxpoles"],
self.nx + 1,
self.ny + 1,
self.nz + 1,
),
dtype=config.get_model_config().materials["dispersivedtype"],
)
def initialise_dispersive_update_coeff_array(self):
"""Initialise array for storing update coefficients when there are dispersive
materials present.
"""
self.updatecoeffsdispersive = np.zeros(
(len(self.materials), 3 * config.get_model_config().materials["maxpoles"]),
dtype=config.get_model_config().materials["dispersivedtype"],
)
def reset_fields(self):
"""Clear arrays for field components and PMLs."""
# Clear arrays for field components
self.initialise_field_arrays()
if config.get_model_config().materials["maxpoles"] > 0:
self.initialise_dispersive_arrays()
# Clear arrays for fields in PML
for pml in self.pmls["slabs"]:
pml.initialise_field_arrays()
def mem_est_basic(self):
"""Estimates the amount of memory (RAM) required for grid arrays.
Returns:
mem_use: int of memory (bytes).
"""
solidarray = self.nx * self.ny * self.nz * np.dtype(np.uint32).itemsize
# 12 x rigidE array components + 6 x rigidH array components
rigidarrays = (12 + 6) * self.nx * self.ny * self.nz * np.dtype(np.int8).itemsize
# 6 x field arrays + 6 x ID arrays
fieldarrays = (
(6 + 6)
* (self.nx + 1)
* (self.ny + 1)
* (self.nz + 1)
* np.dtype(config.sim_config.dtypes["float_or_double"]).itemsize
)
# PML arrays
pmlarrays = 0
for k, v in self.pmls["thickness"].items():
if v > 0:
if "x" in k:
pmlarrays += (v + 1) * self.ny * (self.nz + 1)
pmlarrays += (v + 1) * (self.ny + 1) * self.nz
pmlarrays += v * self.ny * (self.nz + 1)
pmlarrays += v * (self.ny + 1) * self.nz
elif "y" in k:
pmlarrays += self.nx * (v + 1) * (self.nz + 1)
pmlarrays += (self.nx + 1) * (v + 1) * self.nz
pmlarrays += (self.nx + 1) * v * self.nz
pmlarrays += self.nx * v * (self.nz + 1)
elif "z" in k:
pmlarrays += self.nx * (self.ny + 1) * (v + 1)
pmlarrays += (self.nx + 1) * self.ny * (v + 1)
pmlarrays += (self.nx + 1) * self.ny * v
pmlarrays += self.nx * (self.ny + 1) * v
mem_use = int(fieldarrays + solidarray + rigidarrays + pmlarrays)
return mem_use
def mem_est_dispersive(self):
"""Estimates the amount of memory (RAM) required for dispersive grid arrays.
Returns:
mem_use: int of memory (bytes).
"""
mem_use = int(
3
* config.get_model_config().materials["maxpoles"]
* (self.nx + 1)
* (self.ny + 1)
* (self.nz + 1)
* np.dtype(config.get_model_config().materials["dispersivedtype"]).itemsize
)
return mem_use
def mem_est_fractals(self):
"""Estimates the amount of memory (RAM) required to build any objects
which use the FractalVolume/FractalSurface classes.
Returns:
mem_use: int of memory (bytes).
"""
mem_use = 0
for vol in self.fractalvolumes:
mem_use += vol.nx * vol.ny * vol.nz * vol.dtype.itemsize
for surface in vol.fractalsurfaces:
surfacedims = surface.get_surface_dims()
mem_use += surfacedims[0] * surfacedims[1] * surface.dtype.itemsize
return mem_use
def tmx(self):
"""Add PEC boundaries to invariant direction in 2D TMx mode.
N.B. 2D modes are a single cell slice of 3D grid.
"""
# Ey & Ez components
self.ID[1, 0, :, :] = 0
self.ID[1, 1, :, :] = 0
self.ID[2, 0, :, :] = 0
self.ID[2, 1, :, :] = 0
def tmy(self):
"""Add PEC boundaries to invariant direction in 2D TMy mode.
N.B. 2D modes are a single cell slice of 3D grid.
"""
# Ex & Ez components
self.ID[0, :, 0, :] = 0
self.ID[0, :, 1, :] = 0
self.ID[2, :, 0, :] = 0
self.ID[2, :, 1, :] = 0
def tmz(self):
"""Add PEC boundaries to invariant direction in 2D TMz mode.
N.B. 2D modes are a single cell slice of 3D grid.
"""
# Ex & Ey components
self.ID[0, :, :, 0] = 0
self.ID[0, :, :, 1] = 0
self.ID[1, :, :, 0] = 0
self.ID[1, :, :, 1] = 0
def calculate_dt(self):
"""Calculate time step at the CFL limit."""
if config.get_model_config().mode == "2D TMx":
self.dt = 1 / (
config.sim_config.em_consts["c"] * np.sqrt((1 / self.dy**2) + (1 / self.dz**2))
)
elif config.get_model_config().mode == "2D TMy":
self.dt = 1 / (
config.sim_config.em_consts["c"] * np.sqrt((1 / self.dx**2) + (1 / self.dz**2))
)
elif config.get_model_config().mode == "2D TMz":
self.dt = 1 / (
config.sim_config.em_consts["c"] * np.sqrt((1 / self.dx**2) + (1 / self.dy**2))
)
else:
self.dt = 1 / (
config.sim_config.em_consts["c"]
* np.sqrt((1 / self.dx**2) + (1 / self.dy**2) + (1 / self.dz**2))
)
# Round down time step to nearest float with precision one less than
# hardware maximum. Avoids inadvertently exceeding the CFL due to
# binary representation of floating point number.
self.dt = round_value(self.dt, decimalplaces=decimal.getcontext().prec - 1)
def calculate_Ix(self, x: int, y: int, z: int) -> float:
"""Calculates the x-component of current at a grid position.
Args:
x: x coordinate of position in grid
y: y coordinate of position in grid
z: z coordinate of position in grid
"""
if y == 0 or z == 0:
Ix = 0
else:
Ix = self.dy * (self.Hy[x, y, z - 1] - self.Hy[x, y, z]) + self.dz * (
self.Hz[x, y, z] - self.Hz[x, y - 1, z]
)
return Ix
def calculate_Iy(self, x: int, y: int, z: int) -> float:
"""Calculates the y-component of current at a grid position.
Args:
x: x coordinate of position in grid
y: y coordinate of position in grid
z: z coordinate of position in grid
"""
if x == 0 or z == 0:
Iy = 0
else:
Iy = self.dx * (self.Hx[x, y, z] - self.Hx[x, y, z - 1]) + self.dz * (
self.Hz[x - 1, y, z] - self.Hz[x, y, z]
)
return Iy
def calculate_Iz(self, x: int, y: int, z: int) -> float:
"""Calculates the y-component of current at a grid position.
Args:
x: x coordinate of position in grid
y: y coordinate of position in grid
z: z coordinate of position in grid
"""
if x == 0 or y == 0:
Iz = 0
else:
Iz = self.dx * (self.Hx[x, y - 1, z] - self.Hx[x, y, z]) + self.dy * (
self.Hy[x, y, z] - self.Hy[x - 1, y, z]
)
return Iz
def dispersion_analysis(self, iterations: int):
# Check to see if numerical dispersion might be a problem
results = self._dispersion_analysis(iterations)
if results["error"]:
logger.warning(
f"Numerical dispersion analysis [{self.name}] "
f"not carried out as {results['error']}"
)
elif results["N"] < config.get_model_config().numdispersion["mingridsampling"]:
logger.exception(
f"\nNon-physical wave propagation in [{self.name}] "
f"detected. Material '{results['material'].ID}' "
f"has wavelength sampled by {results['N']} cells, "
f"less than required minimum for physical wave "
f"propagation. Maximum significant frequency "
f"estimated as {results['maxfreq']:g}Hz"
)
raise ValueError
elif (
results["deltavp"]
and np.abs(results["deltavp"])
> config.get_model_config().numdispersion["maxnumericaldisp"]
):
logger.warning(
f"[{self.name}] has potentially significant "
f"numerical dispersion. Estimated largest physical "
f"phase-velocity error is {results['deltavp']:.2f}% "
f"in material '{results['material'].ID}' whose "
f"wavelength sampled by {results['N']} cells. "
f"Maximum significant frequency estimated as "
f"{results['maxfreq']:g}Hz\n"
)
elif results["deltavp"]:
logger.info(
f"Numerical dispersion analysis [{self.name}]: "
f"estimated largest physical phase-velocity error is "
f"{results['deltavp']:.2f}% in material '{results['material'].ID}' "
f"whose wavelength sampled by {results['N']} cells. "
f"Maximum significant frequency estimated as "
f"{results['maxfreq']:g}Hz\n"
)
def _dispersion_analysis(self, iterations: int):
"""Analysis of numerical dispersion (Taflove et al, 2005, p112) -
worse case of maximum frequency and minimum wavelength
Args:
G: FDTDGrid class describing a grid in a model.
Returns:
results: dict of results from dispersion analysis.
"""
# deltavp: physical phase velocity error (percentage)
# N: grid sampling density
# material: material with maximum permittivity
# maxfreq: maximum significant frequency
# error: error message
results = {"deltavp": None, "N": None, "material": None, "maxfreq": [], "error": ""}
# Find maximum significant frequency
if self.waveforms:
for waveform in self.waveforms:
if waveform.type in ["sine", "contsine"]:
results["maxfreq"].append(4 * waveform.freq)
elif waveform.type == "impulse":
results["error"] = "impulse waveform used."
elif waveform.type == "user":
results["error"] = "user waveform detected."
else:
# Time to analyse waveform - 4*pulse_width as using entire
# time window can result in demanding FFT
waveform.calculate_coefficients()
iterations = round_value(4 * waveform.chi / self.dt)
iterations = min(iterations, iterations)
waveformvalues = np.zeros(iterations)
for iteration in range(iterations):
waveformvalues[iteration] = waveform.calculate_value(
iteration * self.dt, self.dt
)
# Ensure source waveform is not being overly truncated before attempting any FFT
if np.abs(waveformvalues[-1]) < np.abs(np.amax(waveformvalues)) / 100:
# FFT
freqs, power = fft_power(waveformvalues, self.dt)
# Get frequency for max power
freqmaxpower = np.where(np.isclose(power, 0))[0][0]
# Set maximum frequency to a threshold drop from maximum power, ignoring DC value
try:
freqthres = (
np.where(
power[freqmaxpower:]
< -config.get_model_config().numdispersion["highestfreqthres"]
)[0][0]
+ freqmaxpower
)
results["maxfreq"].append(freqs[freqthres])
except ValueError:
results["error"] = (
"unable to calculate maximum power "
+ "from waveform, most likely due to "
+ "undersampling."
)
# Ignore case where someone is using a waveform with zero amplitude, i.e. on a receiver
elif waveform.amp == 0:
pass
# If waveform is truncated don't do any further analysis
else:
results["error"] = (
"waveform does not fit within specified "
+ "time window and is therefore being truncated."
)
else:
results["error"] = "no waveform detected."
if results["maxfreq"]:
results["maxfreq"] = max(results["maxfreq"])
# Find minimum wavelength (material with maximum permittivity)
maxer = 0
matmaxer = ""
for x in self.materials:
if x.se != float("inf"):
er = x.er
# If there are dispersive materials calculate the complex
# relative permittivity at maximum frequency and take the real part
if x.__class__.__name__ == "DispersiveMaterial":
er = x.calculate_er(results["maxfreq"])
er = er.real
if er > maxer:
maxer = er
matmaxer = x.ID
results["material"] = next(x for x in self.materials if x.ID == matmaxer)
# Minimum velocity
minvelocity = config.c / np.sqrt(maxer)
# Minimum wavelength
minwavelength = minvelocity / results["maxfreq"]
# Maximum spatial step
if "3D" in config.get_model_config().mode:
delta = max(self.dx, self.dy, self.dz)
elif "2D" in config.get_model_config().mode:
if self.nx == 1:
delta = max(self.dy, self.dz)
elif self.ny == 1:
delta = max(self.dx, self.dz)
elif self.nz == 1:
delta = max(self.dx, self.dy)
# Courant stability factor
S = (config.c * self.dt) / delta
# Grid sampling density
results["N"] = minwavelength / delta
# Check grid sampling will result in physical wave propagation
if (
int(np.floor(results["N"]))
>= config.get_model_config().numdispersion["mingridsampling"]
):
# Numerical phase velocity
vp = np.pi / (
results["N"] * np.arcsin((1 / S) * np.sin((np.pi * S) / results["N"]))
)
# Physical phase velocity error (percentage)
results["deltavp"] = (((vp * config.c) - config.c) / config.c) * 100
# Store rounded down value of grid sampling density
results["N"] = int(np.floor(results["N"]))
return results