forked from devitocodes/devito
-
Notifications
You must be signed in to change notification settings - Fork 2
Commit
This commit does not belong to any branch on this repository, and may belong to a fork outside of the repository.
wave: TryAdd example with no Operator
- Loading branch information
1 parent
4b34fc5
commit 7d7e639
Showing
3 changed files
with
170 additions
and
0 deletions.
There are no files selected for viewing
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
This file contains bidirectional Unicode text that may be interpreted or compiled differently than what appears below. To review, open the file in an editor that reveals hidden Unicode characters.
Learn more about bidirectional Unicode characters
Original file line number | Diff line number | Diff line change |
---|---|---|
@@ -0,0 +1,168 @@ | ||
# Based on the implementation of the Devito acoustic example implementation | ||
# Not using Devito's source injection abstraction | ||
import sys | ||
import numpy as np | ||
|
||
from devito import (TimeFunction, Eq, Operator, solve, norm, | ||
XDSLOperator, configuration, Grid) | ||
from examples.seismic import RickerSource | ||
from examples.seismic import Model, TimeAxis, plot_image | ||
from fast.bench_utils import plot_2dfunc | ||
from devito.tools import as_tuple | ||
|
||
import argparse | ||
np.set_printoptions(threshold=np.inf) | ||
|
||
|
||
parser = argparse.ArgumentParser(description='Process arguments.') | ||
|
||
parser.add_argument("-d", "--shape", default=(16, 16), type=int, nargs="+", | ||
help="Number of grid points along each axis") | ||
parser.add_argument("-so", "--space_order", default=4, | ||
type=int, help="Space order of the simulation") | ||
parser.add_argument("-to", "--time_order", default=2, | ||
type=int, help="Time order of the simulation") | ||
parser.add_argument("-nt", "--nt", default=20, | ||
type=int, help="Simulation time in millisecond") | ||
parser.add_argument("-bls", "--blevels", default=1, type=int, nargs="+", | ||
help="Block levels") | ||
parser.add_argument("-plot", "--plot", default=False, type=bool, help="Plot2D") | ||
parser.add_argument("-devito", "--devito", default=False, type=bool, help="Devito run") | ||
parser.add_argument("-xdsl", "--xdsl", default=False, type=bool, help="xDSL run") | ||
args = parser.parse_args() | ||
|
||
|
||
mpiconf = configuration['mpi'] | ||
|
||
# Define a physical size | ||
# nx, ny, nz = args.shape | ||
nt = args.nt | ||
|
||
shape = (args.shape) # Number of grid point (nx, ny, nz) | ||
spacing = as_tuple(10.0 for _ in range(len(shape))) # Grid spacing in m. The domain size is now 1km by 1km | ||
origin = as_tuple(0.0 for _ in range(len(shape))) # What is the location of the top left corner. | ||
domain_size = tuple((d-1) * s for d, s in zip(shape, spacing)) | ||
grid = Grid(shape=shape, extent=(1000, 1000)) | ||
# grid = Grid(shape=shape) | ||
# This is necessary to define | ||
# the absolute location of the source and receivers | ||
|
||
# Define a velocity profile. The velocity is in km/s | ||
v = np.empty(shape, dtype=np.float32) | ||
v[:, :] = 1 | ||
|
||
# With the velocity and model size defined, we can create the seismic model that | ||
# encapsulates this properties. We also define the size of the absorbing layer as | ||
# 10 grid points | ||
so = args.space_order | ||
to = args.time_order | ||
|
||
#model = Model(vp=v, origin=origin, shape=shape, spacing=spacing, | ||
# space_order=so, nbl=0) | ||
|
||
# plot_velocity(model) | ||
|
||
t0 = 0. # Simulation starts a t=0 | ||
tn = nt # Simulation last 1 second (1000 ms) | ||
# dt = model.critical_dt # Time step from model grid spacing | ||
# print("dt is:", dt) | ||
|
||
#time_range = TimeAxis(start=t0, stop=tn, step=dt) | ||
|
||
# The source is positioned at a $20m$ depth and at the middle of the | ||
# $x$ axis ($x_{src}=500m$), | ||
# with a peak wavelet frequency of $10Hz$. | ||
f0 = 0.010 # Source peak frequency is 10Hz (0.010 kHz) | ||
#src = RickerSource(name='src', grid=model.grid, f0=f0, | ||
# npoint=1, time_range=time_range) | ||
|
||
# First, position source centrally in all dimensions, then set depth | ||
#src.coordinates.data[0, :] = np.array(model.domain_size) * .5 | ||
|
||
# We can plot the time signature to see the wavelet | ||
# src.show() | ||
|
||
# Define the wavefield with the size of the model and the time dimension | ||
u = TimeFunction(name="u", grid=grid, time_order=to, space_order=so) | ||
# Another one to clone data | ||
u2 = TimeFunction(name="u", grid=grid, time_order=to, space_order=so) | ||
ub = TimeFunction(name="ub", grid=grid, time_order=to, space_order=so) | ||
|
||
# We can now write the PDE | ||
# pde = model.m * u.dt2 - u.laplace + model.damp * u.dt | ||
# import pdb;pdb.set_trace() | ||
pde = u.dt2 - u.laplace | ||
|
||
stencil = Eq(u.forward, solve(pde, u.forward)) | ||
# stencil | ||
|
||
# Finally we define the source injection and receiver read function to generate | ||
# the corresponding code | ||
# print(time_range) | ||
|
||
#src_term = src.inject(field=u.forward, expr=src * dt**2 / model.m) | ||
#op0 = Operator([stencil] + src_term, subs=model.spacing_map, name='SourceDevitoOperator') | ||
|
||
# Run with source and plot | ||
#op0.apply(time=time_range.num-1, dt=model.critical_dt) | ||
|
||
|
||
|
||
# print("Init Devito linalg norm 0 :", np.linalg.norm(u.data[0])) | ||
# print("Init Devito linalg norm 1 :", np.linalg.norm(u.data[1])) | ||
# print("Init Devito linalg norm 2 :", np.linalg.norm(u.data[2])) | ||
# print("Norm of initial data:", norm(u)) | ||
|
||
configuration['mpi'] = 0 | ||
u2.data[:] = u.data[:] | ||
configuration['mpi'] = mpiconf | ||
|
||
import pdb;pdb.set_trace() | ||
u.data[:] = np.load("wave_dat2.npy", allow_pickle=True) | ||
|
||
if len(shape) == 2: | ||
if args.plot: | ||
plot_2dfunc(u) | ||
|
||
print("Init norm:", np.linalg.norm(u.data[:])) | ||
|
||
if args.devito: | ||
# Run more with no sources now (Not supported in xdsl) | ||
#op1 = Operator([stencil], name='DevitoOperator', subs=grid.spacing_map) | ||
op1 = Operator([stencil], name='DevitoOperator') | ||
op1.apply(time=10, dt=5.54) | ||
|
||
configuration['mpi'] = 0 | ||
ub.data[:] = u.data[:] | ||
configuration['mpi'] = mpiconf | ||
|
||
if len(shape) == 2 and args.plot: | ||
plot_2dfunc(u) | ||
|
||
print("After Operator 1: Devito norm:", norm(u)) | ||
# print("Devito linalg norm 0:", np.linalg.norm(u.data[0])) | ||
# print("Devito linalg norm 1:", np.linalg.norm(u.data[1])) | ||
# print("Devito linalg norm 2:", np.linalg.norm(u.data[2])) | ||
|
||
|
||
if args.xdsl: | ||
# Reset initial data | ||
configuration['mpi'] = 0 | ||
u.data[:] = u2.data[:] | ||
configuration['mpi'] = mpiconf | ||
# v[:, ..., :] = 1 | ||
# print("Reinitialise data: Devito norm:", norm(u)) | ||
# print("XDSL init linalg norm:", np.linalg.norm(u.data[0])) | ||
# print("XDSL init linalg norm:", np.linalg.norm(u.data[1])) | ||
# print("XDSL init linalg norm:", np.linalg.norm(u.data[2])) | ||
|
||
# Run more with no sources now (Not supported in xdsl) | ||
xdslop = Operator([stencil], name='xDSLOperator') | ||
xdslop.apply(time=nt) | ||
|
||
if len(shape) == 2 and args.plot: | ||
plot_2dfunc(u) | ||
|
||
print("XDSL output norm 0:", np.linalg.norm(u.data[0]), "vs:", np.linalg.norm(ub.data[0])) | ||
print("XDSL output norm 1:", np.linalg.norm(u.data[1]), "vs:", np.linalg.norm(ub.data[1])) | ||
print("XDSL output norm 2:", np.linalg.norm(u.data[2]), "vs:", np.linalg.norm(ub.data[2])) |