Note
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Refraction in 3D#
This example shows refracted ray paths in a three-dimensional vertical gradient medium.
Note
This is a placeholder/proof-of-concept. The code should be refactored partly to tt.showRayPaths()
import numpy as np
import pygimli as pg
import pygimli.meshtools as mt
from pygimli.physics import traveltime as tt
from pygimli.viewer.pv import drawSensors
import pyvista
Build mesh.
depth = 15
width = 30
plc = mt.createCube(size=[width, width, depth], pos=[0, 0, -depth/2], area=5)
n_sensors = 8
sensors = np.zeros((n_sensors, 3))
sensors[0, 0] = 15
sensors[0, 1] = -10
sensors[1:, 0] = -15
sensors[1:, 1] = np.linspace(-15, 15, n_sensors - 1)
for pos in sensors:
plc.createNode(pos)
mesh = mt.createMesh(plc)
mesh.createSecondaryNodes(1)
Create vertical gradient model.
vel = 300 + -pg.z(mesh.cellCenters()) * 100
pg.show(mesh, vel, label=pg.utils.unit("vel"), showMesh=True)
(<pyvista.plotting.plotter.Plotter object at 0x7f91162fbc10>, None)
Set-up data container.
Do raytracing.
# fop = pg.core.TravelTimeDijkstraModelling(mesh, data)
fop = tt.TravelTimeModelling()
fop.setData(data)
fop.setMesh(mesh)
print(fop.mesh())
# This is to show single raypaths.
graph = fop.createGraph(1 / vel)
dij = tt.Dijkstra(graph)
dij.setStartNode(mesh.findNearestNode([15, -10, 0]))
rays = []
for receiver in sensors[1:]:
ni = dij.shortestPathTo(mesh.findNearestNode(receiver))
pos = mesh.positions(withSecNodes=True)[ni]
segs = np.zeros((len(pos), 3))
segs[:,0] = pg.x(pos)
segs[:,1] = pg.y(pos)
segs[:,2] = pg.z(pos)
rays.append(segs)
Mesh: Nodes: 1621 Cells: 6906 Boundaries: 14797 secNodes: 24308
Plot final ray paths.
pl, _ = pg.show(mesh, style='wireframe', line_width=0.1,
hold=True)
drawSensors(pl, sensors, diam=0.5, color='yellow')
for ray in rays:
for i in range(len(ray) - 1):
start = tuple(ray[i])
stop = tuple(ray[i + 1])
line = pyvista.Line(start, stop)
pl.add_mesh(line, color='green', line_width=2)
pl.show()