def _testP1_(mesh, show=False, followP2=True):
""" Laplace u = 0
with u = x and u(x=min)=0 and u(x=max)=1
Test for u == exact x for P1 base functions
"""
#print('b', mesh, mesh.cell(0))
u = pg.solve(mesh, a=1, b=0, f=0,
bc={'Dirichlet': {1: 0, 2: 1}})
if show:
if mesh.dim()==1:
pg.plt.figure()
x = pg.x(mesh)
ix = np.argsort(x)
pg.plt.plot(x[ix], u[ix])
elif mesh.dim() > 1:
pg.show(mesh, u, label='u')
xMin = mesh.xMin()
xSpan = (mesh.xMax() - xMin)
np.testing.assert_allclose(u, (pg.x(mesh)-xMin) / xSpan)
if followP2:
_testP2_(mesh, show)
return u
def _testP2_(mesh, show=False):
""" Laplace u - 2 = 0
with u(x) = x² + x/(xMax-xMin) + xMin/(xMax-xMin)
and u(xMin)=0 and u(xMax)=1
Test for u_h === u(x) for P2 base functions
"""
meshP2 = mesh.createP2()
u = pg.solve(
meshP2,
f=-2,
bc={'Dirichlet': {
'1,2': 2
}},
)
xMin = mesh.xMin()
xSpan = (mesh.xMax() - xMin)
if show:
if mesh.dim() == 1:
pg.plt.figure()
x = pg.x(mesh)
ix = np.argsort(x)
pg.plt.plot(x[ix], x[ix]**2 - (xSpan / 2)**2 + 2)
elif mesh.dim() > 1:
pg.show(meshP2, u, label='u = x**2')
np.testing.assert_allclose(u, pg.x(meshP2)**2 - (xSpan / 2)**2 + 2)
def test_Helmholtz(self):
"""
d² u / d x² + k u + f = 0
k = 2
a) P1(exact)
u = x
f = -2x
b) P2(exact)
u = x*x
f = -(2 + 2x*x)
"""
h = np.pi/2 / 21
x = np.arange(0.0, np.pi/2, h)
mesh = pg.createGrid(x)
### test a)
k = 2.0
u = lambda _x: _x
f = lambda _x: -(k * u(_x))
x = pg.x(mesh)
dirichletBC = [[1, u(min(x))], [2, u(max(x))]]
uFEM = pg.solve(mesh, a=1, b=k, f=f(x), bc={'Dirichlet': dirichletBC})
np.testing.assert_allclose(uFEM, u(x))
### test b)
u = lambda _x: _x * _x
f = lambda _x: -(2. + k *u(_x))
mesh = mesh.createP2()
x = pg.x(mesh)
dirichletBC = [[1, u(min(x))], [2, u(max(x))]]
uFEM = pg.solve(mesh, a=1, b=k, f=f(x), bc={'Dirichlet': dirichletBC})
np.testing.assert_allclose(uFEM, u(x), atol=1e-6)
def test_Helmholtz(self):
"""
d² u / d x² + k u + f = 0
k = 2
a) P1(exact)
u = x
f = -2x
b) P2(exact)
u = x*x
f = -(2 + 2x*x)
"""
h = np.pi / 2 / 21
x = np.arange(0.0, np.pi / 2, h)
mesh = pg.createGrid(x)
### test a)
k = 2.0
u = lambda _x: _x
f = lambda _x: -(k * u(_x))
x = pg.x(mesh)
dirichletBC = [[1, u(min(x))], [2, u(max(x))]]
uFEM = pg.solve(mesh, a=1, b=k, f=f(x), bc={'Dirichlet': dirichletBC})
np.testing.assert_allclose(uFEM, u(x))
### test b)
u = lambda _x: _x * _x
f = lambda _x: -(2. + k * u(_x))
mesh = mesh.createP2()
x = pg.x(mesh)
dirichletBC = [[1, u(min(x))], [2, u(max(x))]]
uFEM = pg.solve(mesh, a=1, b=k, f=f(x), bc={'Dirichlet': dirichletBC})
np.testing.assert_allclose(uFEM, u(x), atol=1e-6)
def testShowVariants():
# Create geometry definition for the modelling domain
world = mt.createWorld(start=[-10, 0], end=[10, -16],
layers=[-8], worldMarker=False)
# Create a heterogeneous block
block = mt.createRectangle(start=[-6, -3.5], end=[6, -6.0],
marker=4, boundaryMarker=10, area=0.1)
circ = mt.createCircle(pos=[0, -11], radius=2, boundaryMarker=11, isHole=True)
# Merge geometrical entities
geom = world + block + circ
mesh = mt.createMesh(geom)
fig, axs = plt.subplots(3,5)
pg.show(geom, ax=axs[0][0])
axs[0][0].set_title('plc, (default)')
pg.show(geom, fillRegion=False, ax=axs[0][1])
axs[0][1].set_title('plc, fillRegion=False')
pg.show(geom, showBoundary=False, ax=axs[0][2])
axs[0][2].set_title('plc, showBoundary=False')
pg.show(geom, markers=True, ax=axs[0][3])
axs[0][3].set_title('plc, markers=True')
pg.show(mesh, ax=axs[0][4], showBoundary=False)
axs[0][4].set_title('mesh, showBoundary=False')
pg.show(mesh, ax=axs[1][0])
axs[1][0].set_title('mesh, (default)')
pg.show(mesh, mesh.cellMarkers(), label='Cell markers', ax=axs[1][1])
axs[1][1].set_title('mesh, cells, (default)')
pg.show(mesh, markers=True, ax=axs[1][2])
axs[1][2].set_title('mesh, cells, markers=True')
pg.show(mesh, mesh.cellMarkers(), label='Cell markers', showMesh=True, ax=axs[1][3])
axs[1][3].set_title('mesh, cells, showMesh=True')
pg.show(mesh, mesh.cellMarkers(), label='Cell markers', showBoundary=False, ax=axs[1][4])
axs[1][4].set_title('mesh, cells, showBoundary=False')
pg.show(mesh, pg.x(mesh), label='Nodes (x)', ax=axs[2][0])
axs[2][0].set_title('mesh, nodes, (default)')
pg.show(mesh, pg.x(mesh), label='Nodes (x)', showMesh=True, ax=axs[2][1])
axs[2][1].set_title('mesh, nodes, showMesh=True')
pg.show(mesh, pg.x(mesh), label='Nodes (x)', showBoundary=True, ax=axs[2][2])
axs[2][2].set_title('mesh, nodes, showBoundary=True')
pg.show(mesh, pg.y(mesh.cellCenters()), label='Cell center (y)',
tri=True, shading='flat', ax=axs[2][3])
axs[2][3].set_title('mesh, cells, tri=True, shading=flat')
pg.show(mesh, pg.y(mesh.cellCenters()), label='Cell center (y)',
tri=True, shading='gouraud', ax=axs[2][4])
axs[2][4].set_title('mesh, cells, tri=True, shading=gouraud')
##pg.show(mesh, mesh.cellMarker(), label(markers), axs[1][1])
axs[2][4].figure.tight_layout()
def ani(i):
axGra.clear()
axGra.plot(pg.x(gravPoints), dz[i])
axGra.plot(pg.x(gravPoints), pg.y(gravPoints), 'v', color='black')
axGra.set_ylabel('Grav in mGal')
axGra.set_xlim((-20, 20))
axGra.set_ylim((0, 0.001))
axGra.grid()
pg.mplviewer.setMappableData(gciDDe, abs(dDens[i]),
cMin=0, cMax=20,
logScale=False)
def drawVA(ax, data, vals=None, usePos=True, pseudosection=False, **kwargs):
"""Draw apparent velocities as matrix into an axis.
Parameters
----------
ax : mpl.Axes
data : pg.DataContainer()
Datacontainer with 's' and 'g' Sensorindieces and 't' traveltimes.
usePos: bool [True]
Use sensor positions for axes tick labels
pseudosection : bool [False]
Show in pseudosection style.
vals : iterable
Traveltimes, if None data need to contain 't' values.
"""
if isinstance(vals, str):
vals = data(vals)
if vals is None:
vals = data('t')
px = pg.x(data)
gx = np.asarray([px[g] for g in data.id("g")])
sx = np.asarray([px[s] for s in data.id("s")])
offset = shotReceiverDistances(data, full=True)
if min(vals) < 1e-10:
print(vals)
pg.error('zero traveltimes found.')
va = offset / vals
if pseudosection:
midpoint = (gx + sx) / 2
gci = pg.viewer.mpl.dataview.drawVecMatrix(ax, midpoint, offset, va,
queeze=True,
label=pg.unit('as'))
else:
gci = pg.viewer.mpl.dataview.drawVecMatrix(ax, gx, sx, va,
squeeze=True,
label=pg.unit('as'))
# A = np.ones((data.sensorCount(), data.sensorCount())) * np.nan
# for i in range(data.size()):
# A[int(data('s')[i]), int(data('g')[i])] = va[i]
# gci = ax.imshow(A, interpolation='nearest')
# ax.grid(True)
if usePos:
xt = np.arange(0, data.sensorCount(), 50)
ax.set_xticks(xt)
ax.set_xticklabels([str(int(px[xti])) for xti in xt])
ax.set_yticks(xt)
ax.set_yticklabels([str(int(px[xti])) for xti in xt])
return gci
def create_mesh_and_data(n):
nc = np.linspace(-2.0, 0.0, n)
mesh = pg.createMesh2D(nc, nc)
mcx = pg.x(mesh.cellCenter())
mcy = pg.y(mesh.cellCenter())
data = np.cos(1.5 * mcx) * np.sin(1.5 * mcy)
return mesh, data
def cellDataToBoundaryGrad(mesh, v, vGrad):
"""TODO Documentme."""
if len(v) != mesh.cellCount() or len(vGrad) != mesh.cellCount():
raise BaseException("len(v) dismatch mesh.cellCount()")
gB = mesh.cellDataToBoundaryGradient(v, vGrad)
return np.vstack([pg.x(gB), pg.y(gB), pg.z(gB)]).T
def drawFirstPicks(ax, data, tt=None, plotva=False, **kwargs):
"""Plot first arrivals as lines."""
px = pg.x(data)
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
if tt is None:
tt = np.array(data("t"))
if plotva:
tt = np.absolute(gx - sx) / tt
uns = np.unique(sx)
cols = plt.cm.tab10(np.arange(10))
kwargs.setdefault('marker', 'x')
kwargs.setdefault('markersize', 8)
kwargs.setdefault('linestyle', '-')
for i, si in enumerate(uns):
ti = tt[sx == si]
gi = gx[sx == si]
ii = gi.argsort()
ax.plot(gi[ii], ti[ii], color=cols[i % 10], **kwargs)
ax.plot(si, 0., 's', color=cols[i % 10])
ax.grid(True)
if plotva:
ax.set_ylabel("Apparent velocity (m/s)")
else:
ax.set_ylabel("Traveltime (s)")
ax.set_xlabel("x (m)")
ax.invert_yaxis()
def cellDataToCellGrad(mesh, v, CtB):
"""TODO Documentme."""
if len(v) != mesh.cellCount():
print(len(v), mesh.cellCount())
raise BaseException("len of v missmatch mesh.cellCount()")
div = mesh.boundaryDataToCellGradient(CtB * v)
return np.vstack([pg.x(div), pg.y(div), pg.z(div)]).T
def integrate(f, ent, order):
""" integrate function """
J = 0
x = []
w = []
if type(ent) is list:
a = ent[0]
b = ent[1]
xs = pg.IntegrationRules.instance().gauAbscissa(order)
w = pg.IntegrationRules.instance().gauWeights(order)
x = (b - a) / 2.0 * pg.x(xs) + (a + b) / 2.0
J = (b - a) / 2.
else:
J = ent.shape().jacobianDeterminant()
xs = pg.IntegrationRules.instance().abscissa(ent.shape(), order)
w = pg.IntegrationRules.instance().weights(ent.shape(), order)
x = [ent.shape().xyz(xsi) for xsi in xs]
for xx in x:
print xx
print w
print funct(f)(x)
return J * sum(funct(f)(x) * w)
def cellDataToBoundaryGrad(mesh, v, vGrad):
"""
"""
if len(v) != mesh.cellCount() or len(vGrad) != mesh.cellCount():
raise
gB = mesh.cellDataToBoundaryGradient(v, vGrad)
return np.vstack([pg.x(gB), pg.y(gB), pg.z(gB)]).T
gB = np.zeros((mesh.boundaryCount(), 3))
for b in mesh.boundaries():
leftCell = b.leftCell()
rightCell = b.rightCell()
gr = pg.RVector3(0.0, 0.0, 0.0)
t = (b.node(1).pos() - b.node(0).pos()).norm()
if leftCell and rightCell:
df1 = b.center().distance(leftCell.center())
df2 = b.center().distance(rightCell.center())
gr = b.norm() * \
(v[rightCell.id()] - v[leftCell.id()]) / (df1 + df2)
grL = t * t.dot(vGrad[leftCell.id()])
grR = t * t.dot(vGrad[rightCell.id()])
gr += (grL + grR) * 0.5
elif leftCell:
gr = t * t.dot(vGrad[leftCell.id()])
gB[b.id(), 0] = gr[0]
gB[b.id(), 1] = gr[1]
gB[b.id(), 2] = gr[2]
return gB
def shotReceiverDistances(data, full=False):
"""Return vector of all distances (in m) between shot and receiver.
for each 's' and 'g' in data.
Parameters
----------
data : pg.DataContainerERT
full : bool [False]
Get distances between shot and receiver position when full is True or
only form x coordinate if full is False
Returns
-------
dists : array
Array of distances
"""
if full:
pos = data.sensors()
s, g = data.id("s"), data.id("g")
off = [pos[s[i]].distance(pos[g[i]]) for i in range(data.size())]
return np.absolute(off)
else:
px = pg.x(data)
gx = np.array([px[g] for g in data.id("g")])
sx = np.array([px[s] for s in data.id("s")])
return np.absolute(gx - sx)
def cellDataToBoundaryGrad(mesh, v, vGrad):
"""
"""
if len(v) != mesh.cellCount() or len(vGrad) != mesh.cellCount():
raise
gB = mesh.cellDataToBoundaryGradient(v, vGrad)
return np.vstack([pg.x(gB), pg.y(gB), pg.z(gB)]).T
gB = np.zeros((mesh.boundaryCount(), 3))
for b in mesh.boundaries():
leftCell = b.leftCell()
rightCell = b.rightCell()
gr = pg.RVector3(0.0, 0.0, 0.0)
t = (b.node(1).pos() - b.node(0).pos()).norm()
if leftCell and rightCell:
df1 = b.center().distance(leftCell.center())
df2 = b.center().distance(rightCell.center())
gr = b.norm() * (v[rightCell.id()] - v[leftCell.id()]) / (df1 +
df2)
grL = t * t.dot(vGrad[leftCell.id()])
grR = t * t.dot(vGrad[rightCell.id()])
gr += (grL + grR) * 0.5
elif leftCell:
gr = t * t.dot(vGrad[leftCell.id()])
gB[b.id(), 0] = gr[0]
gB[b.id(), 1] = gr[1]
gB[b.id(), 2] = gr[2]
return gB
def plotFirstPicks(ax, data, tt=None, plotva=False, marker='x-'):
"""plot first arrivals as lines"""
px = pg.x(data.sensorPositions())
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
if tt is None:
tt = np.array(data("t"))
if plotva:
tt = np.absolute(gx - sx) / tt
uns = np.unique(sx)
cols = plt.cm.tab10(np.arange(10))
for i, si in enumerate(uns):
ti = tt[sx == si]
gi = gx[sx == si]
ii = gi.argsort()
ax.plot(gi[ii], ti[ii], marker, color=cols[i % 10])
ax.plot(si, 0., 's', color=cols[i % 10], markersize=8)
ax.grid(True)
if plotva:
ax.set_ylabel("Apparent velocity (m/s)")
else:
ax.set_ylabel("Traveltime (s)")
ax.set_xlabel("x (m)")
ax.invert_yaxis()
def cellDataToCellGrad(mesh, v, CtB):
if len(v) != mesh.cellCount():
print(len(v), mesh.cellCount())
raise
div = mesh.boundaryDataToCellGradient(CtB * v)
return np.vstack([pg.x(div), pg.y(div), pg.z(div)]).T
vF = cellDataToBoundaryData(mesh, v)
gC = np.zeros((mesh.cellCount(), 3))
for b in mesh.boundaries():
leftCell = b.leftCell()
rightCell = b.rightCell()
vec = b.norm() * vF[b.id()] * b.size()
if leftCell:
gC[leftCell.id(), 0] += vec[0]
gC[leftCell.id(), 1] += vec[1]
gC[leftCell.id(), 2] += vec[2]
if rightCell:
gC[rightCell.id(), 0] -= vec[0]
gC[rightCell.id(), 1] -= vec[1]
gC[rightCell.id(), 2] -= vec[2]
gC[:, 0] /= mesh.cellSizes()
gC[:, 1] /= mesh.cellSizes()
gC[:, 2] /= mesh.cellSizes()
return gC
def transform2DMeshTo3D(mesh, x, y, z=None):
"""
Transform a 2D mesh into 3D coordinates using a point list (e.g. from GPS)
Parameters
----------
mesh: GIMLi::Mesh
x,y: array of x/y positions along 2d profile
z: optional height to add (topographical correction if computed flat earth)
See Also
--------
References
----------
"""
# get mesh node positions
mt, mz = pg.x( mesh.positions() ), pg.y( mesh.positions() ) # mesh tape and z
# compute length of reference points along tape
pt = np.hstack( (0., np.cumsum( np.sqrt( np.diff( x )**2 + np.diff( y )**2 ) ) ) )
# interpolate node positions from tape to x/y using tape positions
mx = np.interp( mt, pt, x )
my = np.interp( mt, pt, y )
# compute z offset by interpolating z
if z is None:
oz = np.zeros( len(mt) )
else:
oz = np.interp( mt, pt, z )
# set the positions in the mesh
for i, node in enumerate( mesh.nodes() ):
node.setPos( pg.RVector3( mx[i], my[i], mz[i]+oz[i] ) )
def showVA(self, data=None, t=None, name='va', pseudosection=False,
squeeze=True, full=True, ax=None, cmap=None, **kwargs):
"""Show apparent velocity as image plot.
TODO showXXX commands need to return ax and cbar .. if there is one
"""
if data is None:
data = self.dataContainer
if ax is None:
fig, ax = plt.subplots()
self.figs[name] = fig
self.axs[name] = ax
if t is None:
t = data('t')
px = pg.x(data.sensorPositions())
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
offset = self.getOffset(data=data, full=full)
va = offset / t
if pseudosection:
midpoint = (gx + sx) / 2
showVecMatrix(midpoint, offset, va, squeeze=True, ax=ax,
label='Apparent slowness [s/m]', cmap=cmap, **kwargs)
else:
showVecMatrix(gx, sx, va, squeeze=squeeze, ax=ax,
label='Apparent velocity [m/s]', cmap=cmap, **kwargs)
fig.show()
return ax # va
def create_mesh_and_data(n):
nc = np.linspace(-2.0, 0.0, n)
mesh = pg.createMesh2D(nc, nc)
mcx = pg.x(mesh.cellCenter())
mcy = pg.y(mesh.cellCenter())
data = np.cos(1.5 * mcx) * np.sin(1.5 * mcy)
return mesh, data
def showVA(self, ax=None, t=None, name='va', pseudosection=False,
squeeze=True, full=True):
"""show apparent velocity as image plot
TODO showXXX commands need to return axes and cbar .. if there is one
"""
if ax is None:
fig, ax = plt.subplots()
self.figs[name] = fig
self.axs[name] = ax
if t is None:
t = self.dataContainer('t')
px = pg.x(self.dataContainer.sensorPositions())
gx = np.array([px[int(g)] for g in self.dataContainer("g")])
sx = np.array([px[int(s)] for s in self.dataContainer("s")])
offset = self.getOffset(full=full)
va = offset / t
if pseudosection:
midpoint = (gx + sx) / 2
plotVecMatrix(midpoint, offset, va, squeeze=True, ax=ax,
label='Apparent slowness [s/m]')
else:
plotVecMatrix(gx, sx, va, squeeze=squeeze, ax=ax,
label='Apparent velocity [m/s]')
# va = showVA(ax, self.dataContainer)
# plt.show(block=False)
return va
def integrate(f, ent, order):
""" integrate function """
J = 0
x = []
w = []
if type(ent) is list:
a = ent[0]
b = ent[1]
xs = pg.IntegrationRules.instance().gauAbscissa(order)
w = pg.IntegrationRules.instance().gauWeights(order)
x = (b - a) / 2.0 * pg.x(xs) + (a + b) / 2.0
J = (b - a) / 2.0
else:
J = ent.shape().jacobianDeterminant()
xs = pg.IntegrationRules.instance().abscissa(ent.shape(), order)
w = pg.IntegrationRules.instance().weights(ent.shape(), order)
x = [ent.shape().xyz(xsi) for xsi in xs]
for xx in x:
print xx
print w
print funct(f)(x)
return J * sum(funct(f)(x) * w)
def cellDataToCellGrad(mesh, v, CtB):
if len(v) != mesh.cellCount():
print(len(v), mesh.cellCount())
raise
div = mesh.boundaryDataToCellGradient(CtB * v)
return np.vstack([pg.x(div), pg.y(div), pg.z(div)]).T
vF = cellDataToBoundaryData(mesh, v)
gC = np.zeros((mesh.cellCount(), 3))
for b in mesh.boundaries():
leftCell = b.leftCell()
rightCell = b.rightCell()
vec = b.norm() * vF[b.id()] * b.size()
if leftCell:
gC[leftCell.id(), 0] += vec[0]
gC[leftCell.id(), 1] += vec[1]
gC[leftCell.id(), 2] += vec[2]
if rightCell:
gC[rightCell.id(), 0] -= vec[0]
gC[rightCell.id(), 1] -= vec[1]
gC[rightCell.id(), 2] -= vec[2]
gC[:, 0] /= mesh.cellSizes()
gC[:, 1] /= mesh.cellSizes()
gC[:, 2] /= mesh.cellSizes()
return gC
def cellDataToBoundaryGrad(mesh, v, vGrad):
"""TODO Documentme."""
if len(v) != mesh.cellCount() or len(vGrad) != mesh.cellCount():
raise BaseException("len(v) dismatch mesh.cellCount()")
gB = mesh.cellDataToBoundaryGradient(v, vGrad)
return np.vstack([pg.x(gB), pg.y(gB), pg.z(gB)]).T
def showMesh3DFallback(mesh, data, **kwargs):
"""
Plot the 3D object sketchy.
"""
ax = kwargs.pop('ax', None)
from mpl_toolkits.mplot3d import Axes3D
if ax is None or not isinstance(ax, Axes3D):
fig = plt.figure()
ax = fig.gca(projection='3d', proj_type='persp')
#ax = fig.gca(projection='3d', proj_type='ortho')
if mesh.boundaryCount() > 0:
x, y, tri, z, dataIndex = pg.viewer.mpl.createTriangles(mesh)
ax.plot_trisurf(x, y, tri, z)
else:
if mesh.nodeCount() < 1e4:
x = pg.x(mesh.positions())
y = pg.y(mesh.positions())
z = pg.z(mesh.positions())
ax.scatter(x, y, z, 'ko')
ax.set_title('Fallback, install pyvista for proper 3D visualization')
return ax, None
def cellDataToCellGrad(mesh, v, CtB):
"""TODO Documentme."""
if len(v) != mesh.cellCount():
print(len(v), mesh.cellCount())
raise BaseException("len of v missmatch mesh.cellCount()")
div = mesh.boundaryDataToCellGradient(CtB * v)
return np.vstack([pg.x(div), pg.y(div), pg.z(div)]).T
def createCoarsePoly( coarseData ):
boundary = 1250.0
mesh = g.Mesh()
x = g.x( coarseData )
y = g.y( coarseData )
z = g.z( coarseData )
xMin = min( x ); xMax = max( x )
yMin = min( y ); yMax = max( y )
zMin = min( z ); zMax = max( z )
print(xMin, xMax, yMin, yMax)
border = max( (xMax - xMin) * boundary / 100.0, (yMax - yMin) * boundary / 100.0);
n1 = mesh.createNode( xMin - border, yMin - border, zMin, 1 )
n2 = mesh.createNode( xMax + border, yMin - border, zMin, 2 )
n3 = mesh.createNode( xMax + border, yMax + border, zMin, 3 )
n4 = mesh.createNode( xMin - border, yMax + border, zMin, 4 )
mesh.createEdge( n1, n2, 12 );
mesh.createEdge( n2, n3, 23 );
mesh.createEdge( n3, n4, 34 );
mesh.createEdge( n4, n1, 41 );
for p in coarseData:
mesh.createNode( p )
return mesh
def plotFirstPicks(ax, data, tt=None, plotva=False, marker='x-'):
"""plot first arrivals as lines"""
px = pg.x(data.sensorPositions())
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
if tt is None:
tt = np.array(data("t"))
if plotva:
tt = np.absolute(gx - sx) / tt
uns = np.unique(sx)
cols = plt.cm.tab10(np.arange(10))
for i, si in enumerate(uns):
ti = tt[sx == si]
gi = gx[sx == si]
ii = gi.argsort()
ax.plot(gi[ii], ti[ii], marker, color=cols[i % 10])
ax.plot(si, 0., 's', color=cols[i % 10], markersize=8)
ax.grid(True)
if plotva:
ax.set_ylabel("Apparent velocity (m/s)")
else:
ax.set_ylabel("Traveltime (s)")
ax.set_xlabel("x (m)")
ax.invert_yaxis()
def test_Helmholtz(self):
"""
d² u / d x² + k u + f = 0
k = 2
a) P1(exact)
u = x
f = -k x
b) P2(exact)
u = x*x
f = -(2 + 2x*x)
"""
h = np.pi / 2 / 21
x = np.arange(0.0, np.pi / 2, h)
mesh = pg.createGrid(x)
### test a)
k = 2.0
u = lambda _x: _x
f = lambda _x, _k: -_k * u(_x)
x = pg.x(mesh)
dirichletBC = {1: u(min(x)), 2: u(max(x))}
uFEM = pg.solve(mesh,
a=1,
b=k,
f=f(x, k),
bc={'Dirichlet': dirichletBC})
# pg.plt.plot(x, uFEM, '.')
# pg.plt.plot(pg.sort(x), u(pg.sort(x)))
# pg.wait()
np.testing.assert_allclose(uFEM, u(x))
### test b)
u = lambda _x: _x * _x
f = lambda _x, _k: -(2. + k * u(_x))
mesh = mesh.createP2()
x = pg.x(mesh)
dirichletBC = {1: u(min(x)), 2: u(max(x))}
uFEM = pg.solve(mesh,
a=1,
b=k,
f=f(x, k),
bc={'Dirichlet': dirichletBC})
np.testing.assert_allclose(uFEM, u(x), atol=1e-6)
def createGradientModel2D(data, mesh, vTop, vBot):
"""Create 2D velocity gradient model.
Creates a smooth, linear, starting model that takes the slope
of the topography into account. This is done by fitting a straight line
and using the distance to that as the depth value.
Known as "The Marcus method"
TODO
----
* Cite "The Marcus method"
Parameters
----------
data: pygimli DataContainer
The topography list is in here.
mesh: pygimli.Mesh
The parametric mesh used for the inversion
vTop: float
The velocity at the surface of the mesh
vBot: float
The velocity at the bottom of the mesh
Returns
-------
model: pygimli Vector, length M
A numpy array with slowness values that can be used to start
the inversion.
"""
yVals = pg.y(data)
if abs(min(yVals)) < 1e-8 and abs(max(yVals)) < 1e-8:
yVals = pg.z(data)
p = np.polyfit(pg.x(data), yVals, deg=1) # slope-intercept form
n = np.asarray([-p[0], 1.0]) # normal vector
nLen = np.sqrt(np.dot(n, n))
x = pg.x(mesh.cellCenters())
z = pg.y(mesh.cellCenters())
pos = np.column_stack((x, z))
d = np.array([
np.abs(np.dot(pos[i, :], n) - p[1]) / nLen for i in range(pos.shape[0])
])
return 1.0 / np.interp(d, [min(d), max(d)], [vTop, vBot])
def test_createPartMesh(self):
mesh = pg.meshtools.createMesh1D(np.linspace(0, 1, 10))
self.assertEqual(mesh.cellCount(), 9)
mesh2 = mesh.createMeshByCellIdx(
pg.find(pg.x(mesh.cellCenters()) < 0.5))
self.assertEqual(mesh2.cellCount(), 4)
self.assertEqual(mesh2.cellCenters()[-1][0] < 0.5, True)
def test_createPartMesh(self):
mesh = pg.createMesh1D(np.linspace(0, 1, 10))
self.assertEqual(mesh.cellCount(), 9)
mesh2 = mesh.createMeshByCellIdx(
pg.find(pg.x(mesh.cellCenters()) < 0.5))
self.assertEqual(mesh2.cellCount(), 4)
self.assertEqual(mesh2.cellCenters()[-1][0] < 0.5, True)
def createTriangles(mesh):
"""Generate triangle objects for later drawing.
Creates triangle for each 2D triangle cell or 3D boundary.
Quads will be split into two triangles.
Result will be cached into mesh._triData.
Parameters
----------
mesh : :gimliapi:`GIMLI::Mesh`
2D mesh or 3D mesh
Returns
-------
x : numpy array
x position of nodes
y : numpy array
x position of nodes
triangles : numpy array Cx3
cell indices for each triangle, quad or boundary face
z : numpy array
z position for given indices
dataIdx : list of int
List of indices for a data array
"""
if hasattr(mesh, '_triData'):
if hash(mesh) == mesh._triData[0]:
return mesh._triData[1:]
x = pg.x(mesh)
y = pg.y(mesh)
z = pg.z(mesh)
# x.round(1e-1)
# y.round(1e-1)
if mesh.dim() == 2:
ents = mesh.cells()
else:
ents = mesh.boundaries(mesh.boundaryMarkers() != 0)
if len(ents) == 0:
for b in mesh.boundaries():
if b.leftCell() is None or b.rightCell() is None:
ents.append(b)
triangles = []
dataIdx = []
for c in ents:
triangles.append([c.node(0).id(), c.node(1).id(), c.node(2).id()])
dataIdx.append(c.id())
if c.shape().nodeCount() == 4:
triangles.append([c.node(0).id(), c.node(2).id(), c.node(3).id()])
dataIdx.append(c.id())
mesh._triData = [hash(mesh), x, y, triangles, z, dataIdx]
return x, y, triangles, z, dataIdx
def getMidpoint(self, data=None):
"""Return vector of offsets (in m) between shot and receiver."""
if data is None:
data = self.dataContainer
px = pg.x(data.sensorPositions())
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
return (gx + sx) / 2
def getMidpoint(self, data=None):
"""Return vector of offsets (in m) between shot and receiver."""
if data is None:
data = self.dataContainer
px = pg.x(data.sensorPositions())
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
return (gx + sx) / 2
def _testP1_(mesh, show=False):
""" Laplace u = 0 solves u = x for u(r=0)=0 and u(r=1)=1
Test for u == exact x for P1 base functions
"""
u = pg.solve(mesh, a=1, b=0, f=0,
bc={'Dirichlet': [[1, 0], [2, 1]]})
if show:
if mesh.dim()==1:
pg.plt.plot(pg.x(mesh), u)
pg.wait()
elif mesh.dim()==2:
pg.show(mesh, u, label='u')
pg.wait()
xMin = mesh.xmin()
xSpan = (mesh.xmax() - xMin)
np.testing.assert_allclose(u, (pg.x(mesh)-xMin)/ xSpan)
return u
def _testP1_(mesh, show=False):
""" Laplace u = 0 solves u = x for u(r=0)=0 and u(r=1)=1
Test for u == exact x for P1 base functions
"""
u = pg.solve(mesh, a=1, b=0, f=0,
bc={'Dirichlet': [[1, 0], [2, 1]]})
if show:
if mesh.dim()==1:
pg.plt.plot(pg.x(mesh), u)
pg.wait()
elif mesh.dim()==2:
pg.show(mesh, u, label='u')
pg.wait()
xMin = mesh.xmin()
xSpan = (mesh.xmax() - xMin)
np.testing.assert_allclose(u, (pg.x(mesh)-xMin)/ xSpan)
return u
def calcInvBlock(mesh, dens, out='gravInv'):
# extract block delta density
densBlock = pg.RVector(dens)
densMarker2 = dens[pg.find(mesh.cellMarker() == 2)[0]]
# densBlock[(mesh.cellMarker() == 1)|(mesh.cellMarker() == 3)] = densMarker2
densBlock[pg.find((mesh.cellMarker() == 1) | (mesh.cellMarker() == 3))] = \
densMarker2
densBlock -= densMarker2
# define meausrement positions
gravPointsX = np.linspace(-20, 20, 41)
sensorPositions = np.vstack((gravPointsX, np.zeros(len(gravPointsX)))).T
# solve analytical
gz = solveGravimetry(mesh, densBlock, pnts=sensorPositions, complete=False)
# noisyfy
errAbs = 0.00001
dzerr = np.random.randn(len(sensorPositions)) * errAbs
gz = gz + dzerr
# createParamesh
paraMesh = pg.createGrid(x=np.linspace(-20, 20, 41),
y=np.linspace(-20, 0, 21))
# init Gravimetry manager (should do meshing, simulation and noisying)
Grav = Gravimetry(verbose=True)
model = Grav.invert(sensorPositions, gz, errAbs, verbose=1, mesh=paraMesh)
fig, ax = plt.subplots()
ax.plot(pg.x(sensorPositions), gz, label='gz')
ax.plot(pg.x(sensorPositions), Grav.inv.response(), label='response')
ax.legend()
ax.grid()
ax.set_xlabel('$x$ [m]')
ax.set_ylabel('$\partial u / \partial z$ [mGal]')
plt.show(block=False)
ax.figure.savefig(out, bbox_inches='tight')
return Grav, densBlock
def calcInvBlock(mesh, dens, out='gravInv'):
# extract block delta density
densBlock = pg.RVector(dens)
densMarker2 = dens[pg.find(mesh.cellMarker() == 2)[0]]
#densBlock[(mesh.cellMarker() == 1) | (mesh.cellMarker() == 3)] = densMarker2
densBlock[pg.find((mesh.cellMarker() == 1)
| (mesh.cellMarker() == 3))] = densMarker2
densBlock -= densMarker2
# define meausrement positions
gravPointsX = np.linspace(-20, 20, 41)
sensorPositions = np.vstack((gravPointsX, np.zeros(len(gravPointsX)))).T
# solve analytical
gz = solveGravimetry(mesh, densBlock, pnts=sensorPositions, complete=False)
# noisyfy
errAbs = 0.00001
dzerr = np.random.randn(len(sensorPositions)) * errAbs
gz = gz + dzerr
# createParamesh
paraMesh = pg.createGrid(x=np.linspace(-20, 20, 41),
y=np.linspace(-20, 0, 21))
# init Gravimetry manager (should do meshing, simulation and noisying)
Grav = Gravimetry(verbose=True)
model = Grav.invert(sensorPositions, gz, errAbs, verbose=1, mesh=paraMesh)
fig, ax = plt.subplots()
ax.plot(pg.x(sensorPositions), gz, label='gz')
ax.plot(pg.x(sensorPositions), Grav.inv.response(), label='response')
ax.legend()
ax.grid()
ax.set_xlabel('$x$ [m]')
ax.set_ylabel('$\partial u / \partial z$ [mGal]')
plt.show(block=False)
ax.figure.savefig(out, bbox_inches='tight')
return Grav, densBlock
def showVA(self,
data=None,
t=None,
name='va',
pseudosection=False,
squeeze=True,
full=True,
ax=None,
cmap=None,
**kwargs):
"""Show apparent velocity as image plot.
TODO showXXX commands need to return ax and cbar .. if there is one
"""
if data is None:
data = self.dataContainer
if ax is None:
fig, ax = plt.subplots()
self.figs[name] = fig
self.axs[name] = ax
if t is None:
t = data('t')
px = pg.x(data.sensorPositions())
py = pg.y(data.sensorPositions())
if len(np.unique(py)) > len(np.unique(px)): # probably crosshole
px = py
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
offset = self.getOffset(data=data, full=full)
kwargs.setdefault('vals', offset / t)
if pseudosection:
midpoint = (gx + sx) / 2
_, cb = showVecMatrix(midpoint,
offset,
squeeze=True,
ax=ax,
label='Apparent slowness [s/m]',
cmap=cmap,
**kwargs)
else:
_, cb = showVecMatrix(gx,
sx,
squeeze=squeeze,
ax=ax,
label='Apparent velocity [m/s]',
cmap=cmap,
**kwargs)
ax.figure.show()
return ax, cb
def invertGravimetry(gravPoints, dz):
dzerr = np.random.randn(len(gravPoints)) * 0.0001
dz = dz + dzerr
mesh = pg.createGrid(x=np.linspace(-20, 20, 41), y=np.linspace(-20, 0, 21))
grav = Gravimetry(verbose=True)
model = grav.invert(gravPoints, dz, verbose=1, mesh=mesh)
plt.plot(pg.x(gravPoints), dz)
plt.plot(pg.x(gravPoints), grav.inv.response())
paraDomain = grav.fop.regionManager().paraDomain()
pg.show(paraDomain, model, colorBar=1, hold=1)
pg.showNow()
plt.show()
pass
def tapeMeasureToCoordinates(tape, pos):
"""Interpolate 2D tape measured topography to 2D Cartesian coordinates.
Tape and pos value are expected to be sorted along distance to the orign.
TODO optional smooth curve with harmfit
Parameters
----------
tape : [[x,z]] | [RVector3] | R3Vector
List of tape measured topography points with measured distance (x)
from origin and height (z)
pos : iterable
Query positions along the tape measured profile
Returns
-------
res : ndarray(N, 2)
Same as pos but with interpolated height values.
The Distance between pos points and res (along curve) points remains.
Examples
--------
>>> # no need to import matplotlib. pygimli's show does
>>> import numpy as np
>>> import pygimli as pg
>>> import pygimli.meshtools as mt
>>> elec = np.arange(11.)
>>> topo = np.array([[0., 0.], [3., 2.], [4., 2.], [6., 1.], [10., 1.]])
>>> _= pg.plt.plot(topo[:,0], topo[:,1])
>>> p = mt.tapeMeasureToCoordinates(topo, elec)
>>> pg.plt.gca().plot(p[:,0], p[:,1], 'o') #doctest: +ELLIPSIS
[...]
>>> pg.plt.gca().set_aspect(1)
>>> pg.wait()
"""
if isinstance(tape, pg.R3Vector) or isinstance(tape, pg.stdVectorRVector3):
xTape = pg.x(tape)
zTape = pg.z(tape)
else:
xTape = tape[:, 0]
zTape = tape[:, 1]
t = pg.utils.cumDist(pos)
# print(t)
tTape = pg.utils.cumDist(tape)
xt = np.interp(t, tTape, xTape)
zt = np.interp(t, tTape, zTape)
pg.plt.plot(xTape, zTape)
pg.plt.plot(xt, zt, 'o')
pg.wait()
return np.vstack([xt, zt]).T
def solveDarcy(mesh, k=None, p0=1, verbose=False):
"""Darcy flow."""
if verbose:
print("Solve darcy")
uDir = [
[2, p0], # left aquiver
[3, p0], # left bedrock
#[4, 0], # bottom (paper)
[5, 0], # right bedrock
[6, 0], # right aquiver
[7, 0], # right top
]
p = pg.solver.solve(mesh, a=k, uB=uDir)
vel = -pg.solver.grad(mesh, p) * np.asarray([k, k, k]).T
return mesh, mt.cellDataToNodeData(
mesh,
np.asarray([pg.x(vel),
pg.y(vel)]).T), p, k, np.asarray([pg.x(vel),
pg.y(vel)])
def invertGravimetry(gravPoints, dz):
dzerr = np.random.randn(len(gravPoints)) * 0.0001
dz = dz + dzerr
mesh = pg.createGrid(x=np.linspace(-20, 20, 41),
y=np.linspace(-20, 0, 21))
grav = Gravimetry(verbose=True)
model = grav.invert(gravPoints, dz, verbose=1, mesh=mesh)
plt.plot(pg.x(gravPoints), dz)
plt.plot(pg.x(gravPoints), grav.inv.response())
paraDomain=grav.fop.regionManager().paraDomain()
pg.show(paraDomain, model, colorBar=1, hold=1)
pg.showNow()
plt.show()
pass
def drawTravelTimeData(ax, data, t=None):
"""Draw first arrival traveltime data into mpl ax a.
data of type pg.DataContainer must contain sensorIdx 's' and 'g'
and thus being numbered internally [0..n)
"""
x = pg.x(data.sensorPositions())
# z = pg.z(data.sensorPositions())
shots = pg.unique(pg.sort(data('s')))
geoph = pg.unique(pg.sort(data('g')))
startOffsetIDX = 0
if min(min(shots), min(geoph)) == 1:
startOffsetIDX = 1
tShow = data('t')
if t is not None:
tShow = t
ax.set_xlim([min(x), max(x)])
ax.set_ylim([max(tShow), -0.002])
ax.figure.show()
for shot in shots:
gIdx = pg.find(data('s') == shot)
sensorIdx = [int(i__ - startOffsetIDX) for i__ in data('g')[gIdx]]
ax.plot(x[sensorIdx], tShow[gIdx], 'x-')
yPixel = ax.transData.inverted().transform_point((1, 1))[1] - \
ax.transData.inverted().transform_point((0, 0))[1]
xPixel = ax.transData.inverted().transform_point((1, 1))[0] - \
ax.transData.inverted().transform_point((0, 0))[0]
# draw shot points
ax.plot(x[[int(i__ - startOffsetIDX) for i__ in shots]],
np.zeros(len(shots)) + 8. * yPixel,
'gv',
markersize=8)
# draw geophone points
ax.plot(x[[int(i__ - startOffsetIDX) for i__ in geoph]],
np.zeros(len(geoph)) + 3. * yPixel,
'r^',
markersize=8)
ax.grid()
ax.set_ylim([max(tShow), +16. * yPixel])
ax.set_xlim([min(x) - 5. * xPixel, max(x) + 5. * xPixel])
ax.set_xlabel('x-Coordinate [m]')
ax.set_ylabel('Traveltime [ms]')
def createGradientModel2D(data, mesh, VTop, VBot):
"""
Create 2D velocity gradient model.
Creates a smooth, linear, starting model that takes the slope
of the topography into account. This is done by fitting a straight line
and using the distance to that as the depth value.
Known as "The Marcus method"
Parameters
----------
data : pygimli DataContainer
The topography list is in here.
mesh : pygimli.Mesh
The parametric mesh used for the inversion
VTop : float
The velocity at the surface of the mesh
VBot : float
The velocity at the bottom of the mesh
Returns
-------
model : pygimli Vector, length M
A numpy array with slowness values that can be used to start
the inversion.
"""
p = np.polyfit(pg.x(data.sensorPositions()), pg.y(data.sensorPositions()),
deg=1) # slope-intercept form
n = np.asarray([-p[0], 1.0]) # normal vector
nLen = np.sqrt(np.dot(n, n))
x = pg.x(mesh.cellCenters())
z = pg.y(mesh.cellCenters())
pos = np.column_stack((x, z))
d = np.array([np.abs(np.dot(pos[i, :], n) - p[1]) / nLen
for i in range(pos.shape[0])])
return np.interp(d, [min(d), max(d)], [1.0 / VTop, 1.0 / VBot])
def getOffset(self, full=False):
"""return vector of offsets (in m) between shot and receiver"""
if full:
pos = self.dataContainer.sensorPositions()
s, g = self.dataContainer('s'), self.dataContainer('g')
nd = self.dataContainer.size()
off = [pos[int(s[i])].distance(pos[int(g[i])]) for i in range(nd)]
return np.absolute(off)
else:
px = pg.x(self.dataContainer.sensorPositions())
gx = np.array([px[int(g)] for g in self.dataContainer("g")])
sx = np.array([px[int(s)] for s in self.dataContainer("s")])
return np.absolute(gx - sx)
def getOffset(self, full=False):
"""Return vector of offsets (in m) between shot and receiver."""
if full:
pos = self.dataContainer.sensorPositions()
s, g = self.dataContainer('s'), self.dataContainer('g')
nd = self.dataContainer.size()
off = [pos[int(s[i])].distance(pos[int(g[i])]) for i in range(nd)]
return np.absolute(off)
else:
px = pg.x(self.dataContainer.sensorPositions())
gx = np.array([px[int(g)] for g in self.dataContainer("g")])
sx = np.array([px[int(s)] for s in self.dataContainer("s")])
return np.absolute(gx - sx)
def createTriangles(mesh, data=None):
"""
What is this?
"""
x = pg.x(mesh.positions())
# x.round(1e-1)
y = pg.y(mesh.positions())
# y.round(1e-1)
triCount = 0
for c in mesh.cells():
if c.shape().nodeCount() == 4:
triCount = triCount + 2
else:
triCount = triCount + 1
triangles = np.zeros((triCount, 3))
dataIdx = list(range(triCount))
triCount = 0
for c in mesh.cells():
if c.shape().nodeCount() == 4:
triangles[triCount, 0] = c.node(0).id()
triangles[triCount, 1] = c.node(1).id()
triangles[triCount, 2] = c.node(2).id()
dataIdx[triCount] = c.id()
triCount = triCount + 1
triangles[triCount, 0] = c.node(0).id()
triangles[triCount, 1] = c.node(2).id()
triangles[triCount, 2] = c.node(3).id()
dataIdx[triCount] = c.id()
triCount = triCount + 1
else:
triangles[triCount, 0] = c.node(0).id()
triangles[triCount, 1] = c.node(1).id()
triangles[triCount, 2] = c.node(2).id()
dataIdx[triCount] = c.id()
triCount = triCount + 1
z = None
if data is not None:
if len(data) == mesh.cellCount():
# strange behavior if we just use these slice
z = np.array(data[dataIdx])
else:
z = np.array(data)
return x, y, triangles, z, dataIdx
def drawTravelTimeData(axes, data, t=None):
"""
Draw first arrival traveltime data into mpl axes a.
data of type \ref DataContainer must contain sensorIdx 's' and 'g'
and thus being numbered internally [0..n)
"""
x = pg.x(data.sensorPositions())
# z = pg.z(data.sensorPositions())
shots = pg.unique(pg.sort(data('s')))
geoph = pg.unique(pg.sort(data('g')))
startOffsetIDX = 0
if min(min(shots), min(geoph)) == 1:
startOffsetIDX = 1
tShow = data('t')
if t is not None:
tShow = t
axes.set_xlim([min(x), max(x)])
axes.set_ylim([max(tShow), -0.002])
axes.figure.show()
for shot in shots:
gIdx = pg.find(data('s') == shot)
sensorIdx = [int(i__ - startOffsetIDX) for i__ in data('g')[gIdx]]
axes.plot(x[sensorIdx], tShow[gIdx], 'x-')
yPixel = axes.transData.inverted().transform_point((1, 1))[1] - \
axes.transData.inverted().transform_point((0, 0))[1]
xPixel = axes.transData.inverted().transform_point((1, 1))[0] - \
axes.transData.inverted().transform_point((0, 0))[0]
# draw shot points
axes.plot(x[[int(i__ - startOffsetIDX) for i__ in shots]],
np.zeros(len(shots)) + 8. * yPixel, 'gv', markersize=8)
# draw geophone points
axes.plot(x[[int(i__ - startOffsetIDX) for i__ in geoph]],
np.zeros(len(geoph)) + 3. * yPixel, 'r^', markersize=8)
axes.grid()
axes.set_ylim([max(tShow), +16. * yPixel])
axes.set_xlim([min(x) - 5. * xPixel, max(x) + 5. * xPixel])
axes.set_xlabel('x-Coordinate [m]')
axes.set_ylabel('Traveltime [ms]')
def cellDataToBoundaryData(mesh, vec):
"""
DOCUMENT_ME
"""
if len(data) != mesh.cellCount():
raise BaseException("Dimension mismatch, expecting cellCount(): "
+ str(mesh.cellCount())
+ "got: " + str(len(vec)), str(len(vec[0])))
CtB = mesh.cellToBoundaryInterpolation()
if type(vec) == pg.R3Vector():
return np.array([CtB*pg.x(vec), CtB*pg.y(vec), CtB*pg.z(vec)]).T
else:
return CtB*vec
def cellDataToBoundaryData(mesh, data):
""" TODO DOCUMENT_ME """
if len(data) != mesh.cellCount():
raise BaseException("Dimension mismatch, expecting cellCount(): " +
str(mesh.cellCount()) +
"got: " + str(len(data)), str(len(data[0])))
CtB = mesh.cellToBoundaryInterpolation()
if isinstance(data, pg.R3Vector()):
return np.array([CtB * pg.x(data),
CtB * pg.y(data),
CtB * pg.z(data)]).T
else:
return CtB * data
def solveDarcy(mesh, k=None, p0=1, verbose=False):
"""Darcy flow."""
if verbose:
print("Solve Darcy equation ...")
uDir = [[2, p0], # left aquiver
[3, p0], # left bedrock
# [4, 0], # bottom (paper)
[5, 0], # right bedrock
[6, 0], # right aquiver
[7, 0], # right top
]
p = pg.solver.solve(mesh, a=k, bc={'Dirichlet': uDir}, verbose=True)
vel = -pg.solver.grad(mesh, p) * np.asarray([k, k, k]).T
mvel = mt.cellDataToNodeData(mesh, vel)
return mesh, mvel, p, k, np.asarray([pg.x(vel), pg.y(vel)])
def createFinePoly( coarseMesh, ePos ):
paraBoundary = 10
mesh = g.Mesh()
n1 = None; n2 = None; n3 = None; n4 = None
for n in coarseMesh.nodes():
if n.marker() == 1:
n1 = mesh.createNode( n.pos(), 1 )
elif n.marker() == 2:
n2 = mesh.createNode( n.pos(), 2 )
elif n.marker() == 3:
n3 = mesh.createNode( n.pos(), 3 )
elif n.marker() == 4:
n4 = mesh.createNode( n.pos(), 4 )
mesh.createEdge( n1, n2, 12 );
mesh.createEdge( n2, n3, 23 );
mesh.createEdge( n3, n4, 34 );
mesh.createEdge( n4, n1, 41 );
x = g.x( ePos )
y = g.y( ePos )
z = g.z( ePos )
xMin = min( x ); xMax = max( x )
yMin = min( y ); yMax = max( y )
zMin = min( z ); zMax = max( z )
maxSpan = max( xMax - xMin, yMax - yMin );
borderPara = maxSpan * paraBoundary / 100.0;
n5 = mesh.createNode( xMin - borderPara, yMin - borderPara , 0.0, 5 );
n6 = mesh.createNode( xMax + borderPara, yMin - borderPara , 0.0, 6 );
n7 = mesh.createNode( xMax + borderPara, yMax + borderPara , 0.0, 7 );
n8 = mesh.createNode( xMin - borderPara, yMax + borderPara , 0.0, 8 );
mesh.createEdge( n5, n6, 56 );
mesh.createEdge( n6, n7, 67 );
mesh.createEdge( n7, n8, 78 );
mesh.createEdge( n8, n5, 85 );
for p in ePos:
mesh.createNode( p )
return mesh;
def _test_(mesh, show=False):
vTest = 0.1
u = pg.solve(mesh, a=1, f=0,
bc={'Node': [mesh.findNearestNode([0.0, 0.0]), 0.],
'Neumann': [[1, -vTest], [2, vTest]]}, verbose=0)
if show:
if mesh.dim() == 1:
pg.plt.plot(pg.x(mesh), u)
elif mesh.dim() == 2:
pg.show(grid, pg.abs(v))
pg.show(grid, v, showMesh=1)
pg.wait()
v = pg.solver.grad(mesh, u)
#print("|v|:", min(pg.abs(v)), max(pg.abs(v)), pg.mean(pg.abs(v)))
np.testing.assert_allclose(pg.abs(v), np.ones(mesh.cellCount())*vTest)
return v
def exportHDF5Mesh(mesh, exportname, group='mesh', indices='cell_indices',
pos='coordinates', cells='topology', marker='values'):
"""Writes given :gimliapi:`GIMLI::Mesh` in a hdf5 format file.
3D tetrahedron meshes only! Boundary markers are ignored.
Keywords are explained in :py:mod:`pygimli.meshtools.readHDFS`
"""
h5py = pg.optImport('h5py',
requiredFor='export mesh in .h5 data format')
if not isinstance(mesh, pg.Mesh):
mesh = pg.Mesh(mesh)
# prepare output for writing in hdf data container
pg_pos = mesh.positions()
mesh_pos = np.array((np.array(pg.x(pg_pos)), np.array(pg.y(pg_pos)),
np.array(pg.z(pg_pos)))).T
mesh_cells = np.zeros((mesh.cellCount(), 4)) # hard coded for tetrahedrons
for i, cell in enumerate(mesh.cells()):
mesh_cells[i] = cell.ids()
mesh_indices = np.arange(0, mesh.cellCount() + 1, 1, dtype=np.int64)
mesh_markers = np.array(mesh.cellMarkers())
with h5py.File(exportname, 'w') as out:
for grp in np.atleast_1d(group): # can use more than one group
# writing indices
idx_name = '{}/{}'.format(grp, indices)
out.create_dataset(idx_name, data=mesh_indices, dtype=int)
# writing node positions
pos_name = '{}/{}'.format(grp, pos)
out.create_dataset(pos_name, data=mesh_pos, dtype=float)
# writing cells via indices
cells_name = '{}/{}'.format(grp, cells)
out.create_dataset(cells_name, data=mesh_cells, dtype=int)
# writing marker
marker_name = '{}/{}'.format(grp, marker)
out.create_dataset(marker_name, data=mesh_markers, dtype=int)
out[grp][cells].attrs['celltype'] = np.string_('tetrahedron')
out[grp][cells].attrs.create('partition', [0])
return True
def plotFirstPicks(ax, data, tt=None, plotva=False, marker='x-'):
"""plot first arrivals as lines"""
px = pg.x(data.sensorPositions())
gx = np.array([px[int(g)] for g in data("g")])
sx = np.array([px[int(s)] for s in data("s")])
if tt is None:
tt = np.array(data("t"))
if plotva:
tt = np.absolute(gx - sx) / tt
uns = np.unique(sx)
cols = 'brgcmyk'
for i, si in enumerate(uns):
ti = tt[sx == si]
gi = gx[sx == si]
ii = gi.argsort()
ax.plot(gi[ii], ti[ii], marker, color=cols[i % 7])
ax.plot(si, 0., 's', color=cols[i % 7], markersize=8)
ax.grid(True)
def showVA(ax, data, usepos=True):
"""show apparent velocity as image plot"""
px = pg.x(data.sensorPositions())
gx = np.asarray([px[int(g)] for g in data("g")])
sx = np.asarray([px[int(s)] for s in data("s")])
va = np.absolute(gx - sx) / data('t')
A = np.ones((data.sensorCount(), data.sensorCount())) * np.nan
for i in range(data.size()):
A[int(data('s')[i]), int(data('g')[i])] = va[i]
gci = ax.imshow(A, interpolation='nearest')
ax.grid(True)
xt = np.arange(0, data.sensorCount(), 50)
if usepos:
ax.set_xticks(xt)
ax.set_xticklabels([str(int(px[xti])) for xti in xt])
ax.set_yticks(xt)
ax.set_yticklabels([str(int(px[xti])) for xti in xt])
plt.colorbar(gci, ax=ax)
return va
def createMesh(self, quality=34.6, maxarea=0.1, addpoints=None):
"""Create (inversion) mesh by circumventing PLC"""
data = self.dataContainer
sx = list(pg.x(data.sensorPositions()))
sz = list(pg.y(data.sensorPositions()))
if addpoints is not None:
for po in addpoints:
sx.append(po[0])
sz.append(po[1])
iS = np.argsort(np.arctan2(sx-np.mean(sx), sz-np.mean(sz)))
plc = pg.Mesh(2)
nodes = [plc.createNode(sx[i], sz[i], 0) for i in iS]
for i in range(len(nodes)-1):
plc.createEdge(nodes[i], nodes[i+1])
plc.createEdge(nodes[-1], nodes[0])
tri = pg.TriangleWrapper(plc)
tri.setSwitches("-pzFq"+str(quality)+"a"+str(maxarea))
self.setMesh(tri.generate())