moved to mesh folder.

This commit is contained in:
Rowan Cockett
2013-10-18 17:22:13 -07:00
parent 96ce005c59
commit db694dd780
25 changed files with 703 additions and 27 deletions
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import numpy as np
from SimPEG.utils import mkvc
class BaseMesh(object):
"""
BaseMesh does all the counting you don't want to do.
BaseMesh should be inherited by meshes with a regular structure.
:param numpy.array,list n: number of cells in each direction (dim, )
:param numpy.array,list x0: Origin of the mesh (dim, )
"""
def __init__(self, n, x0=None):
# Check inputs
if x0 is None:
x0 = np.zeros(len(n))
if not len(n) == len(x0):
raise Exception("Dimension mismatch. x0 != len(n)")
if len(n) > 3:
raise Exception("Dimensions higher than 3 are not supported.")
# Ensure x0 & n are 1D vectors
self._n = np.array(n, dtype=int).ravel()
self._x0 = np.array(x0).ravel()
self._dim = len(n)
def x0():
doc = """
Origin of the mesh
:rtype: numpy.array (dim, )
:return: x0
"""
fget = lambda self: self._x0
return locals()
x0 = property(**x0())
def r(self, x, xType='CC', outType='CC', format='V'):
"""
Mesh.r is a quick reshape command that will do the best it can at giving you what you want.
For example, you have a face variable, and you want the x component of it reshaped to a 3D matrix.
Mesh.r can fulfil your dreams::
mesh.r(V, 'F', 'Fx', 'M')
| | | { How: 'M' or ['V'] for a matrix (ndgrid style) or a vector (n x dim) }
| | { What you want: ['CC'], 'N', 'F', 'Fx', 'Fy', 'Fz', 'E', 'Ex', 'Ey', or 'Ez' }
| { What is it: ['CC'], 'N', 'F', 'Fx', 'Fy', 'Fz', 'E', 'Ex', 'Ey', or 'Ez' }
{ The input: as a list or ndarray }
For example::
Xex, Yex, Zex = r(mesh.gridEx, 'Ex', 'Ex', 'M') # Separates each component of the Ex grid into 3 matrices
XedgeVector = r(edgeVector, 'E', 'Ex', 'V') # Given an edge vector, this will return just the part on the x edges as a vector
eX, eY, eZ = r(edgeVector, 'E', 'E', 'V') # Separates each component of the edgeVector into 3 vectors
"""
assert (type(x) == list or type(x) == np.ndarray), "x must be either a list or a ndarray"
assert xType in ['CC', 'N', 'F', 'Fx', 'Fy', 'Fz', 'E', 'Ex', 'Ey', 'Ez'], "xType must be either 'CC', 'N', 'F', 'Fx', 'Fy', 'Fz', 'E', 'Ex', 'Ey', or 'Ez'"
assert outType in ['CC', 'N', 'F', 'Fx', 'Fy', 'Fz', 'E', 'Ex', 'Ey', 'Ez'], "outType must be either 'CC', 'N', 'F', Fx', 'Fy', 'Fz', 'E', 'Ex', 'Ey', or 'Ez'"
assert format in ['M', 'V'], "format must be either 'M' or 'V'"
assert outType[:len(xType)] == xType, "You cannot change types when reshaping."
assert xType in outType, 'You cannot change type of components.'
if type(x) == list:
for i, xi in enumerate(x):
assert type(x) == np.ndarray, "x[%i] must be a numpy array" % i
assert xi.size == x[0].size, "Number of elements in list must not change."
x_array = np.ones((x.size, len(x)))
# Unwrap it and put it in a np array
for i, xi in enumerate(x):
x_array[:, i] = mkvc(xi)
x = x_array
assert type(x) == np.ndarray, "x must be a numpy array"
x = x[:] # make a copy.
xTypeIsFExyz = len(xType) > 1 and xType[0] in ['F', 'E'] and xType[1] in ['x', 'y', 'z']
def outKernal(xx, nn):
"""Returns xx as either a matrix (shape == nn) or a vector."""
if format == 'M':
return xx.reshape(nn, order='F')
elif format == 'V':
return mkvc(xx)
def switchKernal(xx):
"""Switches over the different options."""
if xType in ['CC', 'N']:
nn = (self.n) if xType == 'CC' else (self.n+1)
assert xx.size == np.prod(nn), "Number of elements must not change."
return outKernal(xx, nn)
elif xType in ['F', 'E']:
# This will only deal with components of fields, not full 'F' or 'E'
xx = mkvc(xx) # unwrap it in case it is a matrix
nn = self.nF if xType == 'F' else self.nE
nn = np.r_[0, nn]
nx = [0, 0, 0]
nx[0] = self.nFx if xType == 'F' else self.nEx
nx[1] = self.nFy if xType == 'F' else self.nEy
nx[2] = self.nFz if xType == 'F' else self.nEz
for dim, dimName in enumerate(['x', 'y', 'z']):
if dimName in outType:
assert self.dim > dim, ("Dimensions of mesh not great enough for %s%s", (xType, dimName))
assert xx.size == np.sum(nn), 'Vector is not the right size.'
start = np.sum(nn[:dim+1])
end = np.sum(nn[:dim+2])
return outKernal(xx[start:end], nx[dim])
elif xTypeIsFExyz:
# This will deal with partial components (x, y or z) lying on edges or faces
if 'x' in xType:
nn = self.nFx if 'F' in xType else self.nEx
elif 'y' in xType:
nn = self.nFy if 'F' in xType else self.nEy
elif 'z' in xType:
nn = self.nFz if 'F' in xType else self.nEz
assert xx.size == np.prod(nn), 'Vector is not the right size.'
return outKernal(xx, nn)
# Check if we are dealing with a vector quantity
isVectorQuantity = len(x.shape) == 2 and x.shape[1] == self.dim
if outType in ['F', 'E']:
assert ~isVectorQuantity, 'Not sure what to do with a vector vector quantity..'
outTypeCopy = outType
out = ()
for ii, dirName in enumerate(['x', 'y', 'z'][:self.dim]):
outType = outTypeCopy + dirName
out += (switchKernal(x),)
return out
elif isVectorQuantity:
out = ()
for ii in range(x.shape[1]):
out += (switchKernal(x[:, ii]),)
return out
else:
return switchKernal(x)
def n():
doc = """
Number of Cells in each dimension (array of integers)
:rtype: numpy.array
:return: n
"""
fget = lambda self: self._n
return locals()
n = property(**n())
def dim():
doc = """
The dimension of the mesh (1, 2, or 3).
:rtype: int
:return: dim
"""
fget = lambda self: self._dim
return locals()
dim = property(**dim())
def nCx():
doc = """
Number of cells in the x direction
:rtype: int
:return: nCx
"""
fget = lambda self: self.n[0]
return locals()
nCx = property(**nCx())
def nCy():
doc = """
Number of cells in the y direction
:rtype: int
:return: nCy or None if dim < 2
"""
def fget(self):
if self.dim > 1:
return self.n[1]
else:
return None
return locals()
nCy = property(**nCy())
def nCz():
doc = """Number of cells in the z direction
:rtype: int
:return: nCz or None if dim < 3
"""
def fget(self):
if self.dim > 2:
return self.n[2]
else:
return None
return locals()
nCz = property(**nCz())
def nC():
doc = """
Total number of cells in the model.
:rtype: int
:return: nC
"""
fget = lambda self: np.prod(self.n)
return locals()
nC = property(**nC())
def nNx():
doc = """
Number of nodes in the x-direction
:rtype: int
:return: nNx
"""
fget = lambda self: self.nCx + 1
return locals()
nNx = property(**nNx())
def nNy():
doc = """
Number of noes in the y-direction
:rtype: int
:return: nNy or None if dim < 2
"""
def fget(self):
if self.dim > 1:
return self.n[1] + 1
else:
return None
return locals()
nNy = property(**nNy())
def nNz():
doc = """
Number of nodes in the z-direction
:rtype: int
:return: nNz or None if dim < 3
"""
def fget(self):
if self.dim > 2:
return self.n[2] + 1
else:
return None
return locals()
nNz = property(**nNz())
def nN():
doc = """
Total number of nodes
:rtype: int
:return: nN
"""
fget = lambda self: np.prod(self.n + 1)
return locals()
nN = property(**nN())
def nEx():
doc = """
Number of x-edges in each direction
:rtype: numpy.array (dim, )
:return: nEx
"""
fget = lambda self: np.array([x for x in [self.nCx, self.nNy, self.nNz] if not x is None])
return locals()
nEx = property(**nEx())
def nEy():
doc = """
Number of y-edges in each direction
:rtype: numpy.array (dim, )
:return: nEy or None if dim < 2
"""
def fget(self):
if self.dim > 1:
return np.array([x for x in [self.nNx, self.nCy, self.nNz] if not x is None])
else:
return None
return locals()
nEy = property(**nEy())
def nEz():
doc = """
Number of z-edges in each direction
:rtype: numpy.array (dim, )
:return: nEz or None if dim < 3
"""
def fget(self):
if self.dim > 2:
return np.array([x for x in [self.nNx, self.nNy, self.nCz] if not x is None])
else:
return None
return locals()
nEz = property(**nEz())
def nE():
doc = """
Total number of edges in each direction
:rtype: numpy.array (dim, )
:return: [prod(nEx), prod(nEy), prod(nEz)]
"""
fget = lambda self: np.array([np.prod(x) for x in [self.nEx, self.nEy, self.nEz] if not x is None])
return locals()
nE = property(**nE())
def nFx():
doc = """
Number of x-faces in each direction
:rtype: numpy.array (dim, )
:return: nFx
"""
fget = lambda self: np.array([x for x in [self.nNx, self.nCy, self.nCz] if not x is None])
return locals()
nFx = property(**nFx())
def nFy():
doc = """
Number of y-faces in each direction
:rtype: numpy.array (dim, )
:return: nFy or None if dim < 2
"""
def fget(self):
if self.dim > 1:
return np.array([x for x in [self.nCx, self.nNy, self.nCz] if not x is None])
else:
return None
return locals()
nFy = property(**nFy())
def nFz():
doc = """
Number of z-faces in each direction
:rtype: numpy.array (dim, )
:return: nFz or None if dim < 3
"""
def fget(self):
if self.dim > 2:
return np.array([x for x in [self.nCx, self.nCy, self.nNz] if not x is None])
else:
return None
return locals()
nFz = property(**nFz())
def nF():
doc = """
Total number of faces in each direction
:rtype: numpy.array (dim, )
:return: [prod(nFx), prod(nFy), prod(nFz)]
"""
fget = lambda self: np.array([np.prod(x) for x in [self.nFx, self.nFy, self.nFz] if not x is None])
return locals()
nF = property(**nF())
def normals():
doc = """
Face Normals
:rtype: numpy.array (sum(nF), dim)
:return: normals
"""
def fget(self):
if self.dim == 2:
nX = np.c_[np.ones(self.nF[0]), np.zeros(self.nF[0])]
nY = np.c_[np.zeros(self.nF[1]), np.ones(self.nF[1])]
return np.r_[nX, nY]
elif self.dim == 3:
nX = np.c_[np.ones(self.nF[0]), np.zeros(self.nF[0]), np.zeros(self.nF[0])]
nY = np.c_[np.zeros(self.nF[1]), np.ones(self.nF[1]), np.zeros(self.nF[1])]
nZ = np.c_[np.zeros(self.nF[2]), np.zeros(self.nF[2]), np.ones(self.nF[2])]
return np.r_[nX, nY, nZ]
return locals()
normals = property(**normals())
def tangents():
doc = """
Edge Tangents
:rtype: numpy.array (sum(nE), dim)
:return: normals
"""
def fget(self):
if self.dim == 2:
tX = np.c_[np.ones(self.nE[0]), np.zeros(self.nE[0])]
tY = np.c_[np.zeros(self.nE[1]), np.ones(self.nE[1])]
return np.r_[tX, tY]
elif self.dim == 3:
tX = np.c_[np.ones(self.nE[0]), np.zeros(self.nE[0]), np.zeros(self.nE[0])]
tY = np.c_[np.zeros(self.nE[1]), np.ones(self.nE[1]), np.zeros(self.nE[1])]
tZ = np.c_[np.zeros(self.nE[2]), np.zeros(self.nE[2]), np.ones(self.nE[2])]
return np.r_[tX, tY, tZ]
return locals()
tangents = property(**tangents())
def projectFaceVector(self, fV):
"""
Given a vector, fV, in cartesian coordinates, this will project it onto the mesh using the normals
:param numpy.array fV: face vector with shape (nF, dim)
:rtype: numpy.array with shape (nF, )
:return: projected face vector
"""
assert type(fV) == np.ndarray, 'fV must be an ndarray'
assert len(fV.shape) == 2 and fV.shape[0] == np.sum(self.nF) and fV.shape[1] == self.dim, 'fV must be an ndarray of shape (nF x dim)'
return np.sum(fV*self.normals, 1)
def projectEdgeVector(self, eV):
"""
Given a vector, eV, in cartesian coordinates, this will project it onto the mesh using the tangents
:param numpy.array eV: edge vector with shape (nE, dim)
:rtype: numpy.array with shape (nE, )
:return: projected edge vector
"""
assert type(eV) == np.ndarray, 'eV must be an ndarray'
assert len(eV.shape) == 2 and eV.shape[0] == np.sum(self.nE) and eV.shape[1] == self.dim, 'eV must be an ndarray of shape (nE x dim)'
return np.sum(eV*self.tangents, 1)
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import numpy as np
from scipy import sparse as sp
from SimPEG.utils import mkvc, sdiag, speye, kron3, spzeros
def ddx(n):
"""Define 1D derivatives, inner, this means we go from n+1 to n+1"""
return sp.spdiags((np.ones((n+1, 1))*[-1, 1]).T, [0, 1], n, n+1, format="csr")
def checkBC(bc):
""" Checks if boundary condition 'bc' is valid. """
if(type(bc) is str):
bc = [bc, bc]
assert type(bc) is list, 'bc must be a list'
assert len(bc) == 2, 'bc must have two elements'
for bc_i in bc:
assert type(bc_i) is str, "each bc must be a string"
assert bc_i in ['dirichlet', 'neumann'], "each bc must be either, 'dirichlet' or 'neumann'"
return bc
def ddxCellGrad(n, bc):
"""Create 1D derivative operator from cell-centres to nodes this means we go from n to n+1"""
bc = checkBC(bc)
D = sp.spdiags((np.ones((n+1, 1))*[-1, 1]).T, [-1, 0], n+1, n, format="csr")
# Set the first side
if(bc[0] == 'dirichlet'):
D[0, 0] = 2
elif(bc[0] == 'neumann'):
D[0, 0] = 0
# Set the second side
if(bc[1] == 'dirichlet'):
D[-1, -1] = -2
elif(bc[1] == 'neumann'):
D[-1, -1] = 0
return D
def av(n):
"""Define 1D averaging operator from cell-centres to nodes."""
return sp.spdiags((0.5*np.ones((n+1, 1))*[1, 1]).T, [0, 1], n, n+1, format="csr")
class DiffOperators(object):
"""
Class creates the differential operators that you need!
"""
def __init__(self):
raise Exception('DiffOperators is a base class providing differential operators on meshes and cannot run on its own. Inherit to your favorite Mesh class.')
def faceDiv():
doc = "Construct divergence operator (face-stg to cell-centres)."
def fget(self):
if(self._faceDiv is None):
# The number of cell centers in each direction
n = self.n
# Compute faceDivergence operator on faces
if(self.dim == 1):
D = ddx(n[0])
elif(self.dim == 2):
D1 = sp.kron(speye(n[1]), ddx(n[0]))
D2 = sp.kron(ddx(n[1]), speye(n[0]))
D = sp.hstack((D1, D2), format="csr")
elif(self.dim == 3):
D1 = kron3(speye(n[2]), speye(n[1]), ddx(n[0]))
D2 = kron3(speye(n[2]), ddx(n[1]), speye(n[0]))
D3 = kron3(ddx(n[2]), speye(n[1]), speye(n[0]))
D = sp.hstack((D1, D2, D3), format="csr")
# Compute areas of cell faces & volumes
S = self.area
V = self.vol
self._faceDiv = sdiag(1/V)*D*sdiag(S)
return self._faceDiv
return locals()
_faceDiv = None
faceDiv = property(**faceDiv())
def nodalGrad():
doc = "Construct gradient operator (nodes to edges)."
def fget(self):
if(self._nodalGrad is None):
# The number of cell centers in each direction
n = self.n
# Compute divergence operator on faces
if(self.dim == 1):
G = ddx(n[0])
elif(self.dim == 2):
D1 = sp.kron(speye(n[1]+1), ddx(n[0]))
D2 = sp.kron(ddx(n[1]), speye(n[0]+1))
G = sp.vstack((D1, D2), format="csr")
elif(self.dim == 3):
D1 = kron3(speye(n[2]+1), speye(n[1]+1), ddx(n[0]))
D2 = kron3(speye(n[2]+1), ddx(n[1]), speye(n[0]+1))
D3 = kron3(ddx(n[2]), speye(n[1]+1), speye(n[0]+1))
G = sp.vstack((D1, D2, D3), format="csr")
# Compute lengths of cell edges
L = self.edge
self._nodalGrad = sdiag(1/L)*G
return self._nodalGrad
return locals()
_nodalGrad = None
nodalGrad = property(**nodalGrad())
def setCellGradBC(self, BC):
"""
Function that sets the boundary conditions for cell-centred derivative operators.
Examples::
BC = 'neumann' # Neumann in all directions
BC = ['neumann', 'dirichlet', 'neumann'] # 3D, Dirichlet in y Neumann else
BC = [['neumann', 'dirichlet'], 'dirichlet', 'dirichlet'] # 3D, Neumann in x on bottom of domain,
# Dirichlet else
"""
if(type(BC) is str):
BC = [BC for _ in self.n] # Repeat the str self.dim times
elif(type(BC) is list):
assert len(BC) == self.dim, 'BC list must be the size of your mesh'
else:
raise Exception("BC must be a str or a list.")
for i, bc_i in enumerate(BC):
BC[i] = checkBC(bc_i)
self._cellGrad = None # ensure we create a new gradient next time we call it
self._cellGradBC = BC
return BC
_cellGradBC = 'neumann'
def cellGrad():
doc = "The cell centered Gradient, takes you to cell faces."
def fget(self):
if(self._cellGrad is None):
BC = self.setCellGradBC(self._cellGradBC)
n = self.n
if(self.dim == 1):
G = ddxCellGrad(n[0], BC[0])
elif(self.dim == 2):
G1 = sp.kron(speye(n[1]), ddxCellGrad(n[0], BC[0]))
G2 = sp.kron(ddxCellGrad(n[1], BC[1]), speye(n[0]))
G = sp.vstack((G1, G2), format="csr")
elif(self.dim == 3):
G1 = kron3(speye(n[2]), speye(n[1]), ddxCellGrad(n[0], BC[0]))
G2 = kron3(speye(n[2]), ddxCellGrad(n[1], BC[1]), speye(n[0]))
G3 = kron3(ddxCellGrad(n[2], BC[2]), speye(n[1]), speye(n[0]))
G = sp.vstack((G1, G2, G3), format="csr")
# Compute areas of cell faces & volumes
S = self.area
V = self.vol
self._cellGrad = sdiag(S)*G*sdiag(1/V)
return self._cellGrad
return locals()
_cellGrad = None
cellGrad = property(**cellGrad())
def edgeCurl():
doc = "Construct the 3D curl operator."
def fget(self):
if(self._edgeCurl is None):
# The number of cell centers in each direction
n1 = self.nCx
n2 = self.nCy
n3 = self.nCz
# Compute lengths of cell edges
L = self.edge
# Compute areas of cell faces
S = self.area
# Compute divergence operator on faces
d1 = ddx(n1)
d2 = ddx(n2)
d3 = ddx(n3)
D32 = kron3(d3, speye(n2), speye(n1+1))
D23 = kron3(speye(n3), d2, speye(n1+1))
D31 = kron3(d3, speye(n2+1), speye(n1))
D13 = kron3(speye(n3), speye(n2+1), d1)
D21 = kron3(speye(n3+1), d2, speye(n1))
D12 = kron3(speye(n3+1), speye(n2), d1)
O1 = spzeros(np.shape(D32)[0], np.shape(D31)[1])
O2 = spzeros(np.shape(D31)[0], np.shape(D32)[1])
O3 = spzeros(np.shape(D21)[0], np.shape(D13)[1])
C = sp.vstack((sp.hstack((O1, -D32, D23)),
sp.hstack((D31, O2, -D13)),
sp.hstack((-D21, D12, O3))), format="csr")
self._edgeCurl = sdiag(1/S)*(C*sdiag(L))
return self._edgeCurl
return locals()
_edgeCurl = None
edgeCurl = property(**edgeCurl())
def aveF2CC():
doc = "Construct the averaging operator on cell faces to cell centers."
def fget(self):
if(self._aveF2CC is None):
n = self.n
if(self.dim == 1):
self._aveF2CC = av(n[0])
elif(self.dim == 2):
self._aveF2CC = sp.hstack((sp.kron(speye(n[1]), av(n[0])),
sp.kron(av(n[1]), speye(n[0]))), format="csr")
elif(self.dim == 3):
self._aveF2CC = sp.hstack((kron3(speye(n[2]), speye(n[1]), av(n[0])),
kron3(speye(n[2]), av(n[1]), speye(n[0])),
kron3(av(n[2]), speye(n[1]), speye(n[0]))), format="csr")
return self._aveF2CC
return locals()
_aveF2CC = None
aveF2CC = property(**aveF2CC())
def aveE2CC():
doc = "Construct the averaging operator on cell edges to cell centers."
def fget(self):
if(self._aveE2CC is None):
# The number of cell centers in each direction
n = self.n
if(self.dim == 1):
raise Exception('Edge Averaging does not make sense in 1D: Use Identity?')
elif(self.dim == 2):
self._aveE2CC = sp.hstack((sp.kron(av(n[1]), speye(n[0])),
sp.kron(speye(n[1]), av(n[0]))), format="csr")
elif(self.dim == 3):
self._aveE2CC = sp.hstack((kron3(av(n[2]), av(n[1]), speye(n[0])),
kron3(av(n[2]), speye(n[1]), av(n[0])),
kron3(speye(n[2]), av(n[1]), av(n[0]))), format="csr")
return self._aveE2CC
return locals()
_aveE2CC = None
aveE2CC = property(**aveE2CC())
def aveN2CC():
doc = "Construct the averaging operator on cell nodes to cell centers."
def fget(self):
if(self._aveN2CC is None):
# The number of cell centers in each direction
n = self.n
if(self.dim == 1):
self._aveN2CC = av(n[0])
elif(self.dim == 2):
self._aveN2CC = sp.hstack((sp.kron(av(n[1]), av(n[0])),
sp.kron(av(n[1]), av(n[0]))), format="csr")
elif(self.dim == 3):
self._aveN2CC = sp.hstack((kron3(av(n[2]), av(n[1]), av(n[0])),
kron3(av(n[2]), av(n[1]), av(n[0])),
kron3(av(n[2]), av(n[1]), av(n[0]))), format="csr")
return self._aveN2CC
return locals()
_aveN2CC = None
aveN2CC = property(**aveN2CC())
def aveN2CCv():
doc = "Construct the averaging operator on cell nodes to cell centers, keeping each dimension separate."
def fget(self):
if(self._aveN2CCv is None):
# The number of cell centers in each direction
n = self.n
if(self.dim == 1):
self._aveN2CCv = av(n[0])
elif(self.dim == 2):
self._aveN2CCv = sp.block_diag((sp.kron(av(n[1]), av(n[0])),
sp.kron(av(n[1]), av(n[0]))), format="csr")
elif(self.dim == 3):
self._aveN2CCv = sp.block_diag((kron3(av(n[2]), av(n[1]), av(n[0])),
kron3(av(n[2]), av(n[1]), av(n[0])),
kron3(av(n[2]), av(n[1]), av(n[0]))), format="csr")
return self._aveN2CCv
return locals()
_aveN2CCv = None
aveN2CCv = property(**aveN2CCv())
def getMass(self, materialProp=None, loc='e'):
""" Produces mass matricies.
:param str loc: Average to location: 'e'-edges, 'f'-faces
:param None,float,numpy.ndarray materialProp: property to be averaged (see below)
:rtype: scipy.sparse.csr.csr_matrix
:return: M, the mass matrix
materialProp can be::
None -> takes materialProp = 1 (default)
float -> a constant value for entire domain
numpy.ndarray -> if materialProp.size == self.nC
3D property model
if materialProp.size = self.nCz
1D (layered eath) property model
"""
if materialProp is None:
materialProp = np.ones(self.nC)
elif type(materialProp) is float:
materialProp = np.ones(self.nC)*materialProp
elif materialProp.shape == (self.nCz,):
materialProp = materialProp.repeat(self.nCx*self.nCy)
materialProp = mkvc(materialProp)
assert materialProp.shape == (self.nC,), "materialProp incorrect shape"
if loc=='e':
Av = self.aveE2CC
elif loc=='f':
Av = self.aveF2CC
else:
raise ValueError('Invalid loc')
diag = Av.T * (self.vol * mkvc(materialProp))
return sdiag(diag)
def getEdgeMass(self, materialProp=None):
"""mass matrix for products of edge functions w'*M(materialProp)*e"""
return self.getMass(loc='e', materialProp=materialProp)
def getFaceMass(self, materialProp=None):
"""mass matrix for products of face functions w'*M(materialProp)*f"""
return self.getMass(loc='f', materialProp=materialProp)
def getFaceMassDeriv(self):
Av = self.aveF2CC
return Av.T * sdiag(self.vol)
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@@ -0,0 +1,554 @@
from scipy import sparse as sp
from SimPEG.utils import sub2ind, ndgrid, mkvc, getSubArray, sdiag, inv3X3BlockDiagonal, inv2X2BlockDiagonal
import numpy as np
class InnerProducts(object):
"""
Class creates the inner product matrices that you need!
InnerProducts is a base class providing inner product matrices for meshes and cannot run on its own. Inherit to your favorite Mesh class.
**Example problem for DC resistivity**
.. math::
\sigma^{-1}\mathbf{J} = \\nabla \phi
We can define in weak form by integrating with a general face function F:
.. math::
\int_{\\text{cell}}{\sigma^{-1}\mathbf{J} \cdot \mathbf{F}} = \int_{\\text{cell}}{\\nabla \phi \cdot \mathbf{F}}
\int_{\\text{cell}}{\sigma^{-1}\mathbf{J} \cdot \mathbf{F}} = \int_{\\text{cell}}{(\\nabla \cdot \mathbf{F}) \phi } + \int_{\partial \\text{cell}}{ \phi \mathbf{F} \cdot \mathbf{n}}
We can then discretize for every cell:
.. math::
v_{\\text{cell}} \sigma^{-1} (\mathbf{J}_x \mathbf{F}_x +\mathbf{J}_y \mathbf{F}_y + \mathbf{J}_z \mathbf{F}_z ) = -\phi^{\\top} v_{\\text{cell}} (\mathbf{D}_{\\text{cell}} \mathbf{F}) + \\text{BC}
We can represent this in vector form (again this is for every cell), and will generalize for the case of anisotropic (tensor) sigma.
.. math::
\mathbf{F}_c^{\\top} (\sqrt{v_{\\text{cell}}} \Sigma^{-1} \sqrt{v_{\\text{cell}}}) \mathbf{J}_c = -\phi^{\\top} v_{\\text{cell}}( v_\\text{cell}^{-1} \mathbf{D}_{\\text{cell}} \mathbf{A} \mathbf{F}) + \\text{BC}
We multiply by volume on each side of the tensor conductivity to keep symmetry in the system. Here J_c is the Cartesian J (on the faces) and must be calculated differently depending on the mesh:
.. math::
\mathbf{J}_c = \mathbf{Q}_{(i)}\mathbf{J}_\\text{TENSOR} = \mathbf{N}_{(i)}^{-1}\mathbf{Q}_{(i)}\mathbf{J}_\\text{LOM}
Here the i index refers to where we choose to approximate this integral.
We will approximate this relation at every node of the cell, there are 8 in 3D, using a projection matrix Q_i to pick the appropriate fluxes.
We will then average to the cell center. For the TENSOR mesh, this looks like:
.. math::
\mathbf{F}^{\\top}
{1\over 8}
\left(\sum_{i=1}^8
\mathbf{Q}_{(i)}^{-\\top} \sqrt{v_{\\text{cell}}} \Sigma^{-1} \sqrt{v_{\\text{cell}}} \mathbf{Q}_{(i)}
\\right)
\mathbf{J}
=
-\mathbf{F}^{\\top} \mathbf{A} \mathbf{D}_{\\text{cell}}^{\\top} \phi + \\text{BC}
\mathbf{M}(\Sigma^{-1}) \mathbf{J}
=
-\mathbf{A} \mathbf{D}_{\\text{cell}}^{\\top} \phi + \\text{BC}
\mathbf{M}(\Sigma^{-1}) = {1\over 8}
\left(\sum_{i=1}^8
\mathbf{Q}_{(i)}^{-\\top} \sqrt{v_{\\text{cell}}} \Sigma^{-1} \sqrt{v_{\\text{cell}}} \mathbf{Q}_{(i)}
\\right)
The M is returned if mu is set equal to \Sigma^{-1}.
If requested (returnP=True) the projection matricies are returned as well (ordered by nodes).
Here each P (3*nC, sum(nF)) is a combination of the projection, volume, and any normalization to Cartesian coordinates:
.. math::
\mathbf{P}_{(i)} = \sqrt{ {1\over 8} v_{\\text{cell}}} \overbrace{\mathbf{N}_{(i)}^{-1}}^{\\text{LOM only}} \mathbf{Q}_{(i)}
Note that this is completed for each cell in the mesh at the same time.
"""
def __init__(self):
raise Exception('InnerProducts is a base class providing inner product matrices for meshes and cannot run on its own. Inherit to your favorite Mesh class.')
def getFaceInnerProduct(self, mu=None, returnP=False):
"""Wrapper function,
:py:func:`SimPEG.InnerProducts.getEdgeInnerProduct`
:py:func:`SimPEG.InnerProducts.getEdgeInnerProduct2D`
"""
if self.dim == 2:
return getFaceInnerProduct2D(self, mu, returnP)
elif self.dim == 3:
return getFaceInnerProduct(self, mu, returnP)
def getEdgeInnerProduct(self, sigma=None, returnP=False):
"""Wrapper function,
:py:func:`SimPEG.InnerProducts.getFaceInnerProduct`
:py:func:`SimPEG.InnerProducts.getFaceInnerProduct2D`
"""
if self.dim == 2:
return getEdgeInnerProduct2D(self, sigma, returnP)
elif self.dim == 3:
return getEdgeInnerProduct(self, sigma, returnP)
# ------------------------ Geometries ------------------------------
#
#
# node(i,j,k+1) ------ edge2(i,j,k+1) ----- node(i,j+1,k+1)
# / /
# / / |
# edge3(i,j,k) face1(i,j,k) edge3(i,j+1,k)
# / / |
# / / |
# node(i,j,k) ------ edge2(i,j,k) ----- node(i,j+1,k)
# | | |
# | | node(i+1,j+1,k+1)
# | | /
# edge1(i,j,k) face3(i,j,k) edge1(i,j+1,k)
# | | /
# | | /
# | |/
# node(i+1,j,k) ------ edge2(i+1,j,k) ----- node(i+1,j+1,k)
def getFaceInnerProduct(mesh, mu=None, returnP=False):
"""
:param numpy.array mu: material property (tensor properties are possible) at each cell center (nC, (1, 3, or 6))
:param bool returnP: returns the projection matrices
:rtype: scipy.csr_matrix
:return: M, the inner product matrix (sum(nF), sum(nF))
Depending on the number of columns (either 1, 3, or 6) of mu, the material property is interpreted as follows:
.. math::
\\vec{\mu} = \left[\\begin{matrix} \mu_{1} & 0 & 0 \\\\ 0 & \mu_{1} & 0 \\\\ 0 & 0 & \mu_{1} \end{matrix}\\right]
\\vec{\mu} = \left[\\begin{matrix} \mu_{1} & 0 & 0 \\\\ 0 & \mu_{2} & 0 \\\\ 0 & 0 & \mu_{3} \end{matrix}\\right]
\\vec{\mu} = \left[\\begin{matrix} \mu_{1} & \mu_{4} & \mu_{5} \\\\ \mu_{4} & \mu_{2} & \mu_{6} \\\\ \mu_{5} & \mu_{6} & \mu_{3} \end{matrix}\\right]
\mathbf{M}(\\vec{\mu}) = {1\over 8}
\left(\sum_{i=1}^8
\mathbf{J}_c^{-\\top} \sqrt{v_{\\text{cell}}} \\vec{\mu} \sqrt{v_{\\text{cell}}} \mathbf{J}_c
\\right)
If requested (returnP=True) the projection matricies are returned as well (ordered by nodes)::
P = [P000, P001, P010, P011, P100, P101, P110, P111]
Here each P (3*nC, sum(nF)) is a combination of the projection, volume, and any normalization to Cartesian coordinates:
.. math::
\mathbf{P}_{(i)} = \sqrt{ {1\over 8} v_{\\text{cell}}} \overbrace{\mathbf{N}_{(i)}^{-1}}^{\\text{LOM only}} \mathbf{Q}_{(i)}
Note that this is completed for each cell in the mesh at the same time.
"""
if mu is None: # default is ones
mu = np.ones((mesh.nC, 1))
m = np.array([mesh.nCx, mesh.nCy, mesh.nCz])
nc = mesh.nC
i, j, k = np.int64(range(m[0])), np.int64(range(m[1])), np.int64(range(m[2]))
iijjkk = ndgrid(i, j, k)
ii, jj, kk = iijjkk[:, 0], iijjkk[:, 1], iijjkk[:, 2]
if mesh._meshType == 'LOM':
fN1 = mesh.r(mesh.normals, 'F', 'Fx', 'M')
fN2 = mesh.r(mesh.normals, 'F', 'Fy', 'M')
fN3 = mesh.r(mesh.normals, 'F', 'Fz', 'M')
def Pxxx(pos):
ind1 = sub2ind(mesh.nFx, np.c_[ii + pos[0][0], jj + pos[0][1], kk + pos[0][2]])
ind2 = sub2ind(mesh.nFy, np.c_[ii + pos[1][0], jj + pos[1][1], kk + pos[1][2]]) + mesh.nF[0]
ind3 = sub2ind(mesh.nFz, np.c_[ii + pos[2][0], jj + pos[2][1], kk + pos[2][2]]) + mesh.nF[0] + mesh.nF[1]
IND = np.r_[ind1, ind2, ind3].flatten()
PXXX = sp.coo_matrix((np.ones(3*nc), (range(3*nc), IND)), shape=(3*nc, np.sum(mesh.nF))).tocsr()
if mesh._meshType == 'LOM':
I3x3 = inv3X3BlockDiagonal(getSubArray(fN1[0], [i + pos[0][0], j + pos[0][1], k + pos[0][2]]), getSubArray(fN1[1], [i + pos[0][0], j + pos[0][1], k + pos[0][2]]), getSubArray(fN1[2], [i + pos[0][0], j + pos[0][1], k + pos[0][2]]),
getSubArray(fN2[0], [i + pos[1][0], j + pos[1][1], k + pos[1][2]]), getSubArray(fN2[1], [i + pos[1][0], j + pos[1][1], k + pos[1][2]]), getSubArray(fN2[2], [i + pos[1][0], j + pos[1][1], k + pos[1][2]]),
getSubArray(fN3[0], [i + pos[2][0], j + pos[2][1], k + pos[2][2]]), getSubArray(fN3[1], [i + pos[2][0], j + pos[2][1], k + pos[2][2]]), getSubArray(fN3[2], [i + pos[2][0], j + pos[2][1], k + pos[2][2]]))
PXXX = I3x3 * PXXX
return PXXX
# no | node | f1 | f2 | f3
# 000 | i ,j ,k | i , j, k | i, j , k | i, j, k
# 100 | i+1,j ,k | i+1, j, k | i, j , k | i, j, k
# 010 | i ,j+1,k | i , j, k | i, j+1, k | i, j, k
# 110 | i+1,j+1,k | i+1, j, k | i, j+1, k | i, j, k
# 001 | i ,j ,k+1 | i , j, k | i, j , k | i, j, k+1
# 101 | i+1,j ,k+1 | i+1, j, k | i, j , k | i, j, k+1
# 011 | i ,j+1,k+1 | i , j, k | i, j+1, k | i, j, k+1
# 111 | i+1,j+1,k+1 | i+1, j, k | i, j+1, k | i, j, k+1
# Square root of cell volume multiplied by 1/8
v = np.sqrt(0.125*mesh.vol)
V3 = sdiag(np.r_[v, v, v]) # We will multiply on each side to keep symmetry
P000 = V3*Pxxx([[0, 0, 0], [0, 0, 0], [0, 0, 0]])
P100 = V3*Pxxx([[1, 0, 0], [0, 0, 0], [0, 0, 0]])
P010 = V3*Pxxx([[0, 0, 0], [0, 1, 0], [0, 0, 0]])
P110 = V3*Pxxx([[1, 0, 0], [0, 1, 0], [0, 0, 0]])
P001 = V3*Pxxx([[0, 0, 0], [0, 0, 0], [0, 0, 1]])
P101 = V3*Pxxx([[1, 0, 0], [0, 0, 0], [0, 0, 1]])
P011 = V3*Pxxx([[0, 0, 0], [0, 1, 0], [0, 0, 1]])
P111 = V3*Pxxx([[1, 0, 0], [0, 1, 0], [0, 0, 1]])
if mu.size == mesh.nC: # Isotropic!
mu = mkvc(mu) # ensure it is a vector.
Mu = sdiag(np.r_[mu, mu, mu])
elif mu.shape[1] == 3: # Diagonal tensor
Mu = sdiag(np.r_[mu[:, 0], mu[:, 1], mu[:, 2]])
elif mu.shape[1] == 6: # Fully anisotropic
row1 = sp.hstack((sdiag(mu[:, 0]), sdiag(mu[:, 3]), sdiag(mu[:, 4])))
row2 = sp.hstack((sdiag(mu[:, 3]), sdiag(mu[:, 1]), sdiag(mu[:, 5])))
row3 = sp.hstack((sdiag(mu[:, 4]), sdiag(mu[:, 5]), sdiag(mu[:, 2])))
Mu = sp.vstack((row1, row2, row3))
A = P000.T*Mu*P000 + P001.T*Mu*P001 + P010.T*Mu*P010 + P011.T*Mu*P011 + P100.T*Mu*P100 + P101.T*Mu*P101 + P110.T*Mu*P110 + P111.T*Mu*P111
P = [P000, P001, P010, P011, P100, P101, P110, P111]
if returnP:
return A, P
else:
return A
def getFaceInnerProduct2D(mesh, mu=None, returnP=False):
"""
:param numpy.array mu: material property (tensor properties are possible) at each cell center (nC, (1, 2, or 3))
:param bool returnP: returns the projection matrices
:rtype: scipy.csr_matrix
:return: M, the inner product matrix (sum(nF), sum(nF))
Depending on the number of columns (either 1, 2, or 3) of mu, the material property is interpreted as follows:
.. math::
\\vec{\mu} = \left[\\begin{matrix} \mu_{1} & 0 \\\\ 0 & \mu_{1} \end{matrix}\\right]
\\vec{\mu} = \left[\\begin{matrix} \mu_{1} & 0 \\\\ 0 & \mu_{2} \end{matrix}\\right]
\\vec{\mu} = \left[\\begin{matrix} \mu_{1} & \mu_{3} \\\\ \mu_{3} & \mu_{2} \end{matrix}\\right]
.. math::
\mathbf{M}(\\vec{\mu}) = {1\over 4}
\left(\sum_{i=1}^4
\mathbf{J}_c^{-\\top} \sqrt{v_{\\text{cell}}} \\vec{\mu} \sqrt{v_{\\text{cell}}} \mathbf{J}_c
\\right)
If requested (returnP=True) the projection matricies are returned as well (ordered by nodes)::
P = [P00, P10, P01, P11]
Here each P (2*nC, sum(nF)) is a combination of the projection, volume, and any normalization to Cartesian coordinates:
.. math::
\mathbf{P}_{(i)} = \sqrt{ {1\over 4} v_{\\text{cell}}} \overbrace{\mathbf{N}_{(i)}^{-1}}^{\\text{LOM only}} \mathbf{Q}_{(i)}
Note that this is completed for each cell in the mesh at the same time.
"""
if mu is None: # default is ones
mu = np.ones((mesh.nC, 1))
m = np.array([mesh.nCx, mesh.nCy])
nc = mesh.nC
i, j = np.int64(range(m[0])), np.int64(range(m[1]))
iijj = ndgrid(i, j)
ii, jj = iijj[:, 0], iijj[:, 1]
if mesh._meshType == 'LOM':
fN1 = mesh.r(mesh.normals, 'F', 'Fx', 'M')
fN2 = mesh.r(mesh.normals, 'F', 'Fy', 'M')
def Pxx(pos):
ind1 = sub2ind(mesh.nFx, np.c_[ii + pos[0][0], jj + pos[0][1]])
ind2 = sub2ind(mesh.nFy, np.c_[ii + pos[1][0], jj + pos[1][1]]) + mesh.nF[0]
IND = np.r_[ind1, ind2].flatten()
PXX = sp.coo_matrix((np.ones(2*nc), (range(2*nc), IND)), shape=(2*nc, np.sum(mesh.nF))).tocsr()
if mesh._meshType == 'LOM':
I2x2 = inv2X2BlockDiagonal(getSubArray(fN1[0], [i + pos[0][0], j + pos[0][1]]), getSubArray(fN1[1], [i + pos[0][0], j + pos[0][1]]),
getSubArray(fN2[0], [i + pos[1][0], j + pos[1][1]]), getSubArray(fN2[1], [i + pos[1][0], j + pos[1][1]]))
PXX = I2x2 * PXX
return PXX
# no | node | f1 | f2
# 00 | i ,j | i , j | i, j
# 10 | i+1,j | i+1, j | i, j
# 01 | i ,j+1 | i , j | i, j+1
# 11 | i+1,j+1 | i+1, j | i, j+1
# Square root of cell volume multiplied by 1/4
v = np.sqrt(0.25*mesh.vol)
V2 = sdiag(np.r_[v, v]) # We will multiply on each side to keep symmetry
P00 = V2*Pxx([[0, 0], [0, 0]])
P10 = V2*Pxx([[1, 0], [0, 0]])
P01 = V2*Pxx([[0, 0], [0, 1]])
P11 = V2*Pxx([[1, 0], [0, 1]])
if mu.size == mesh.nC: # Isotropic!
mu = mkvc(mu) # ensure it is a vector.
Mu = sdiag(np.r_[mu, mu])
elif mu.shape[1] == 2: # Diagonal tensor
Mu = sdiag(np.r_[mu[:, 0], mu[:, 1]])
elif mu.shape[1] == 3: # Fully anisotropic
row1 = sp.hstack((sdiag(mu[:, 0]), sdiag(mu[:, 2])))
row2 = sp.hstack((sdiag(mu[:, 2]), sdiag(mu[:, 1])))
Mu = sp.vstack((row1, row2))
A = P00.T*Mu*P00 + P10.T*Mu*P10 + P01.T*Mu*P01 + P11.T*Mu*P11
P = [P00, P10, P01, P11]
if returnP:
return A, P
else:
return A
def getEdgeInnerProduct(mesh, sigma=None, returnP=False):
"""
:param numpy.array sigma: material property (tensor properties are possible) at each cell center (nC, (1, 3, or 6))
:param bool returnP: returns the projection matrices
:rtype: scipy.csr_matrix
:return: M, the inner product matrix (sum(nE), sum(nE))
Depending on the number of columns (either 1, 3, or 6) of sigma, the material property is interpreted as follows:
.. math::
\Sigma = \left[\\begin{matrix} \sigma_{1} & 0 & 0 \\\\ 0 & \sigma_{1} & 0 \\\\ 0 & 0 & \sigma_{1} \end{matrix}\\right]
\Sigma = \left[\\begin{matrix} \sigma_{1} & 0 & 0 \\\\ 0 & \sigma_{2} & 0 \\\\ 0 & 0 & \sigma_{3} \end{matrix}\\right]
\Sigma = \left[\\begin{matrix} \sigma_{1} & \sigma_{4} & \sigma_{5} \\\\ \sigma_{4} & \sigma_{2} & \sigma_{6} \\\\ \sigma_{5} & \sigma_{6} & \sigma_{3} \end{matrix}\\right]
What is returned:
.. math::
\mathbf{M}(\Sigma) = {1\over 8}
\left(\sum_{i=1}^8
\mathbf{J}_c^{-\\top} \sqrt{v_{\\text{cell}}} \Sigma \sqrt{v_{\\text{cell}}} \mathbf{J}_c
\\right)
If requested (returnP=True) the projection matricies are returned as well (ordered by nodes)::
P = [P000, P001, P010, P011, P100, P101, P110, P111]
Here each P (3*nC, sum(nE)) is a combination of the projection, volume, and any normalization to Cartesian coordinates:
.. math::
\mathbf{P}_{(i)} = \sqrt{ {1\over 8} v_{\\text{cell}}} \overbrace{\mathbf{N}_{(i)}^{-1}}^{\\text{LOM only}} \mathbf{Q}_{(i)}
Note that this is completed for each cell in the mesh at the same time.
"""
if sigma is None: # default is ones
sigma = np.ones((mesh.nC, 1))
m = np.array([mesh.nCx, mesh.nCy, mesh.nCz])
nc = mesh.nC
i, j, k = np.int64(range(m[0])), np.int64(range(m[1])), np.int64(range(m[2]))
iijjkk = ndgrid(i, j, k)
ii, jj, kk = iijjkk[:, 0], iijjkk[:, 1], iijjkk[:, 2]
if mesh._meshType == 'LOM':
eT1 = mesh.r(mesh.tangents, 'E', 'Ex', 'M')
eT2 = mesh.r(mesh.tangents, 'E', 'Ey', 'M')
eT3 = mesh.r(mesh.tangents, 'E', 'Ez', 'M')
def Pxxx(pos):
ind1 = sub2ind(mesh.nEx, np.c_[ii + pos[0][0], jj + pos[0][1], kk + pos[0][2]])
ind2 = sub2ind(mesh.nEy, np.c_[ii + pos[1][0], jj + pos[1][1], kk + pos[1][2]]) + mesh.nE[0]
ind3 = sub2ind(mesh.nEz, np.c_[ii + pos[2][0], jj + pos[2][1], kk + pos[2][2]]) + mesh.nE[0] + mesh.nE[1]
IND = np.r_[ind1, ind2, ind3].flatten()
PXXX = sp.coo_matrix((np.ones(3*nc), (range(3*nc), IND)), shape=(3*nc, np.sum(mesh.nE))).tocsr()
if mesh._meshType == 'LOM':
I3x3 = inv3X3BlockDiagonal(getSubArray(eT1[0], [i + pos[0][0], j + pos[0][1], k + pos[0][2]]), getSubArray(eT1[1], [i + pos[0][0], j + pos[0][1], k + pos[0][2]]), getSubArray(eT1[2], [i + pos[0][0], j + pos[0][1], k + pos[0][2]]),
getSubArray(eT2[0], [i + pos[1][0], j + pos[1][1], k + pos[1][2]]), getSubArray(eT2[1], [i + pos[1][0], j + pos[1][1], k + pos[1][2]]), getSubArray(eT2[2], [i + pos[1][0], j + pos[1][1], k + pos[1][2]]),
getSubArray(eT3[0], [i + pos[2][0], j + pos[2][1], k + pos[2][2]]), getSubArray(eT3[1], [i + pos[2][0], j + pos[2][1], k + pos[2][2]]), getSubArray(eT3[2], [i + pos[2][0], j + pos[2][1], k + pos[2][2]]))
PXXX = I3x3 * PXXX
return PXXX
# no | node | e1 | e2 | e3
# 000 | i ,j ,k | i ,j ,k | i ,j ,k | i ,j ,k
# 100 | i+1,j ,k | i ,j ,k | i+1,j ,k | i+1,j ,k
# 010 | i ,j+1,k | i ,j+1,k | i ,j ,k | i ,j+1,k
# 110 | i+1,j+1,k | i ,j+1,k | i+1,j ,k | i+1,j+1,k
# 001 | i ,j ,k+1 | i ,j ,k+1 | i ,j ,k+1 | i ,j ,k
# 101 | i+1,j ,k+1 | i ,j ,k+1 | i+1,j ,k+1 | i+1,j ,k
# 011 | i ,j+1,k+1 | i ,j+1,k+1 | i ,j ,k+1 | i ,j+1,k
# 111 | i+1,j+1,k+1 | i ,j+1,k+1 | i+1,j ,k+1 | i+1,j+1,k
# Square root of cell volume multiplied by 1/8
v = np.sqrt(0.125*mesh.vol)
V3 = sdiag(np.r_[v, v, v]) # We will multiply on each side to keep symmetry
P000 = V3*Pxxx([[0, 0, 0], [0, 0, 0], [0, 0, 0]])
P100 = V3*Pxxx([[0, 0, 0], [1, 0, 0], [1, 0, 0]])
P010 = V3*Pxxx([[0, 1, 0], [0, 0, 0], [0, 1, 0]])
P110 = V3*Pxxx([[0, 1, 0], [1, 0, 0], [1, 1, 0]])
P001 = V3*Pxxx([[0, 0, 1], [0, 0, 1], [0, 0, 0]])
P101 = V3*Pxxx([[0, 0, 1], [1, 0, 1], [1, 0, 0]])
P011 = V3*Pxxx([[0, 1, 1], [0, 0, 1], [0, 1, 0]])
P111 = V3*Pxxx([[0, 1, 1], [1, 0, 1], [1, 1, 0]])
if sigma.size == mesh.nC: # Isotropic!
sigma = mkvc(sigma) # ensure it is a vector.
Sigma = sdiag(np.r_[sigma, sigma, sigma])
elif sigma.shape[1] == 3: # Diagonal tensor
Sigma = sdiag(np.r_[sigma[:, 0], sigma[:, 1], sigma[:, 2]])
elif sigma.shape[1] == 6: # Fully anisotropic
row1 = sp.hstack((sdiag(sigma[:, 0]), sdiag(sigma[:, 3]), sdiag(sigma[:, 4])))
row2 = sp.hstack((sdiag(sigma[:, 3]), sdiag(sigma[:, 1]), sdiag(sigma[:, 5])))
row3 = sp.hstack((sdiag(sigma[:, 4]), sdiag(sigma[:, 5]), sdiag(sigma[:, 2])))
Sigma = sp.vstack((row1, row2, row3))
A = P000.T*Sigma*P000 + P001.T*Sigma*P001 + P010.T*Sigma*P010 + P011.T*Sigma*P011 + P100.T*Sigma*P100 + P101.T*Sigma*P101 + P110.T*Sigma*P110 + P111.T*Sigma*P111
P = [P000, P001, P010, P011, P100, P101, P110, P111]
if returnP:
return A, P
else:
return A
def getEdgeInnerProduct2D(mesh, sigma=None, returnP=False):
"""
:param numpy.array sigma: material property (tensor properties are possible) at each cell center (nC, (1, 2, or 3))
:param bool returnP: returns the projection matrices
:rtype: scipy.csr_matrix
:return: M, the inner product matrix (sum(nE), sum(nE))
Depending on the number of columns (either 1, 2, or 3) of sigma, the material property is interpreted as follows:
.. math::
\Sigma = \left[\\begin{matrix} \sigma_{1} & 0 \\\\ 0 & \sigma_{1} \end{matrix}\\right]
\Sigma = \left[\\begin{matrix} \sigma_{1} & 0 \\\\ 0 & \sigma_{2} \end{matrix}\\right]
\Sigma = \left[\\begin{matrix} \sigma_{1} & \sigma_{3} \\\\ \sigma_{3} & \sigma_{2} \end{matrix}\\right]
.. math::
\mathbf{M}(\Sigma) = {1\over 4}
\left(\sum_{i=1}^4
\mathbf{J}_c^{-\\top} \sqrt{v_{\\text{cell}}} \Sigma \sqrt{v_{\\text{cell}}} \mathbf{J}_c
\\right)
If requested (returnP=True) the projection matricies are returned as well (ordered by nodes)::
P = [P00, P10, P01, P11]
Here each P (2*nC, sum(nE)) is a combination of the projection, volume, and any normalization to Cartesian coordinates:
.. math::
\mathbf{P}_{(i)} = \sqrt{ {1\over 4} v_{\\text{cell}}} \overbrace{\mathbf{N}_{(i)}^{-1}}^{\\text{LOM only}} \mathbf{Q}_{(i)}
Note that this is completed for each cell in the mesh at the same time.
"""
if sigma is None: # default is ones
sigma = np.ones((mesh.nC, 1))
m = np.array([mesh.nCx, mesh.nCy])
nc = mesh.nC
i, j = np.int64(range(m[0])), np.int64(range(m[1]))
iijj = ndgrid(i, j)
ii, jj = iijj[:, 0], iijj[:, 1]
if mesh._meshType == 'LOM':
eT1 = mesh.r(mesh.tangents, 'E', 'Ex', 'M')
eT2 = mesh.r(mesh.tangents, 'E', 'Ey', 'M')
def Pxx(pos):
ind1 = sub2ind(mesh.nEx, np.c_[ii + pos[0][0], jj + pos[0][1]])
ind2 = sub2ind(mesh.nEy, np.c_[ii + pos[1][0], jj + pos[1][1]]) + mesh.nE[0]
IND = np.r_[ind1, ind2].flatten()
PXX = sp.coo_matrix((np.ones(2*nc), (range(2*nc), IND)), shape=(2*nc, np.sum(mesh.nE))).tocsr()
if mesh._meshType == 'LOM':
I2x2 = inv2X2BlockDiagonal(getSubArray(eT1[0], [i + pos[0][0], j + pos[0][1]]), getSubArray(eT1[1], [i + pos[0][0], j + pos[0][1]]),
getSubArray(eT2[0], [i + pos[1][0], j + pos[1][1]]), getSubArray(eT2[1], [i + pos[1][0], j + pos[1][1]]))
PXX = I2x2 * PXX
return PXX
# no | node | e1 | e2
# 00 | i ,j | i ,j | i ,j
# 10 | i+1,j | i ,j | i+1,j
# 01 | i ,j+1 | i ,j+1 | i ,j
# 11 | i+1,j+1 | i ,j+1 | i+1,j
# Square root of cell volume multiplied by 1/4
v = np.sqrt(0.25*mesh.vol)
V2 = sdiag(np.r_[v, v]) # We will multiply on each side to keep symmetry
P00 = V2*Pxx([[0, 0], [0, 0]])
P10 = V2*Pxx([[0, 0], [1, 0]])
P01 = V2*Pxx([[0, 1], [0, 0]])
P11 = V2*Pxx([[0, 1], [1, 0]])
if sigma.size == mesh.nC: # Isotropic!
sigma = mkvc(sigma) # ensure it is a vector.
Sigma = sdiag(np.r_[sigma, sigma])
elif sigma.shape[1] == 2: # Diagonal tensor
Sigma = sdiag(np.r_[sigma[:, 0], sigma[:, 1]])
elif sigma.shape[1] == 3: # Fully anisotropic
row1 = sp.hstack((sdiag(sigma[:, 0]), sdiag(sigma[:, 2])))
row2 = sp.hstack((sdiag(sigma[:, 2]), sdiag(sigma[:, 1])))
Sigma = sp.vstack((row1, row2))
A = P00.T*Sigma*P00 + P10.T*Sigma*P10 + P01.T*Sigma*P01 + P11.T*Sigma*P11
P = [P00, P10, P01, P11]
if returnP:
return A, P
else:
return A
if __name__ == '__main__':
from TensorMesh import TensorMesh
h = [np.array([1, 2, 3, 4]), np.array([1, 2, 1, 4, 2]), np.array([1, 1, 4, 1])]
mesh = TensorMesh(h)
mu = np.ones((mesh.nC, 6))
A, P = mesh.getFaceInnerProduct(mu, returnP=True)
B, P = mesh.getEdgeInnerProduct(mu, returnP=True)
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import numpy as np
from BaseMesh import BaseMesh
from DiffOperators import DiffOperators
from InnerProducts import InnerProducts
from LomView import LomView
from SimPEG.utils import mkvc, ndgrid, volTetra, indexCube, faceInfo
# Some helper functions.
length2D = lambda x: (x[:, 0]**2 + x[:, 1]**2)**0.5
length3D = lambda x: (x[:, 0]**2 + x[:, 1]**2 + x[:, 2]**2)**0.5
normalize2D = lambda x: x/np.kron(np.ones((1, 2)), mkvc(length2D(x), 2))
normalize3D = lambda x: x/np.kron(np.ones((1, 3)), mkvc(length3D(x), 2))
class LogicallyOrthogonalMesh(BaseMesh, DiffOperators, InnerProducts, LomView):
"""
LogicallyOrthogonalMesh is a mesh class that deals with logically orthogonal meshes.
Example of a logically orthogonal mesh:
.. plot:: examples/mesh/plot_LogicallyOrthogonalMesh.py
"""
_meshType = 'LOM'
def __init__(self, nodes):
assert type(nodes) == list, "'nodes' variable must be a list of np.ndarray"
for i, nodes_i in enumerate(nodes):
assert type(nodes_i) == np.ndarray, ("nodes[%i] is not a numpy array." % i)
assert nodes_i.shape == nodes[0].shape, ("nodes[%i] is not the same shape as nodes[0]" % i)
assert len(nodes[0].shape) == len(nodes), "Dimension mismatch"
assert len(nodes[0].shape) > 1, "Not worth using LOM for a 1D mesh."
super(LogicallyOrthogonalMesh, self).__init__(np.array(nodes[0].shape)-1, None)
# Save nodes to private variable _gridN as vectors
self._gridN = np.ones((nodes[0].size, self.dim))
for i, node_i in enumerate(nodes):
self._gridN[:, i] = mkvc(node_i)
def gridCC():
doc = "Cell-centered grid."
def fget(self):
if self._gridCC is None:
ccV = (self.aveN2CCv*mkvc(self.gridN))
self._gridCC = ccV.reshape((-1, self.dim), order='F')
return self._gridCC
return locals()
_gridCC = None # Store grid by default
gridCC = property(**gridCC())
def gridN():
doc = "Nodal grid."
def fget(self):
if self._gridN is None:
raise Exception("Someone deleted this. I blame you.")
return self._gridN
return locals()
_gridN = None # Store grid by default
gridN = property(**gridN())
def gridFx():
doc = "Face staggered grid in the x direction."
def fget(self):
if self._gridFx is None:
N = self.r(self.gridN, 'N', 'N', 'M')
if self.dim == 2:
XY = [mkvc(0.5 * (n[:, :-1] + n[:, 1:])) for n in N]
self._gridFx = np.c_[XY[0], XY[1]]
elif self.dim == 3:
XYZ = [mkvc(0.25 * (n[:, :-1, :-1] + n[:, :-1, 1:] + n[:, 1:, :-1] + n[:, 1:, 1:])) for n in N]
self._gridFx = np.c_[XYZ[0], XYZ[1], XYZ[2]]
return self._gridFx
return locals()
_gridFx = None # Store grid by default
gridFx = property(**gridFx())
def gridFy():
doc = "Face staggered grid in the y direction."
def fget(self):
if self._gridFy is None:
N = self.r(self.gridN, 'N', 'N', 'M')
if self.dim == 2:
XY = [mkvc(0.5 * (n[:-1, :] + n[1:, :])) for n in N]
self._gridFy = np.c_[XY[0], XY[1]]
elif self.dim == 3:
XYZ = [mkvc(0.25 * (n[:-1, :, :-1] + n[:-1, :, 1:] + n[1:, :, :-1] + n[1:, :, 1:])) for n in N]
self._gridFy = np.c_[XYZ[0], XYZ[1], XYZ[2]]
return self._gridFy
return locals()
_gridFy = None # Store grid by default
gridFy = property(**gridFy())
def gridFz():
doc = "Face staggered grid in the z direction."
def fget(self):
if self._gridFz is None and self.dim == 3:
N = self.r(self.gridN, 'N', 'N', 'M')
XYZ = [mkvc(0.25 * (n[:-1, :-1, :] + n[:-1, 1:, :] + n[1:, :-1, :] + n[1:, 1:, :])) for n in N]
self._gridFz = np.c_[XYZ[0], XYZ[1], XYZ[2]]
return self._gridFz
return locals()
_gridFz = None # Store grid by default
gridFz = property(**gridFz())
def gridEx():
doc = "Edge staggered grid in the x direction."
def fget(self):
if self._gridEx is None:
N = self.r(self.gridN, 'N', 'N', 'M')
if self.dim == 2:
XY = [mkvc(0.5 * (n[:-1, :] + n[1:, :])) for n in N]
self._gridEx = np.c_[XY[0], XY[1]]
elif self.dim == 3:
XYZ = [mkvc(0.5 * (n[:-1, :, :] + n[1:, :, :])) for n in N]
self._gridEx = np.c_[XYZ[0], XYZ[1], XYZ[2]]
return self._gridEx
return locals()
_gridEx = None # Store grid by default
gridEx = property(**gridEx())
def gridEy():
doc = "Edge staggered grid in the y direction."
def fget(self):
if self._gridEy is None:
N = self.r(self.gridN, 'N', 'N', 'M')
if self.dim == 2:
XY = [mkvc(0.5 * (n[:, :-1] + n[:, 1:])) for n in N]
self._gridEy = np.c_[XY[0], XY[1]]
elif self.dim == 3:
XYZ = [mkvc(0.5 * (n[:, :-1, :] + n[:, 1:, :])) for n in N]
self._gridEy = np.c_[XYZ[0], XYZ[1], XYZ[2]]
return self._gridEy
return locals()
_gridEy = None # Store grid by default
gridEy = property(**gridEy())
def gridEz():
doc = "Edge staggered grid in the z direction."
def fget(self):
if self._gridEz is None and self.dim == 3:
N = self.r(self.gridN, 'N', 'N', 'M')
XYZ = [mkvc(0.5 * (n[:, :, :-1] + n[:, :, 1:])) for n in N]
self._gridEz = np.c_[XYZ[0], XYZ[1], XYZ[2]]
return self._gridEz
return locals()
_gridEz = None # Store grid by default
gridEz = property(**gridEz())
# --------------- Geometries ---------------------
#
#
# ------------------- 2D -------------------------
#
# node(i,j) node(i,j+1)
# A -------------- B
# | |
# | cell(i,j) |
# | I |
# | |
# D -------------- C
# node(i+1,j) node(i+1,j+1)
#
# ------------------- 3D -------------------------
#
#
# node(i,j,k+1) node(i,j+1,k+1)
# E --------------- F
# /| / |
# / | / |
# / | / |
# node(i,j,k) node(i,j+1,k)
# A -------------- B |
# | H ----------|---- G
# | /cell(i,j) | /
# | / I | /
# | / | /
# D -------------- C
# node(i+1,j,k) node(i+1,j+1,k)
def vol():
doc = "Construct cell volumes of the 3D model as 1d array."
def fget(self):
if(self._vol is None):
if self.dim == 2:
A, B, C, D = indexCube('ABCD', self.n+1)
normal, area = faceInfo(np.c_[self.gridN, np.zeros((self.nN, 1))], A, B, C, D)
self._vol = area
elif self.dim == 3:
# Each polyhedron can be decomposed into 5 tetrahedrons
# However, this presents a choice so we may as well divide in two ways and average.
A, B, C, D, E, F, G, H = indexCube('ABCDEFGH', self.n+1)
vol1 = (volTetra(self.gridN, A, B, D, E) + # cutted edge top
volTetra(self.gridN, B, E, F, G) + # cutted edge top
volTetra(self.gridN, B, D, E, G) + # middle
volTetra(self.gridN, B, C, D, G) + # cutted edge bottom
volTetra(self.gridN, D, E, G, H)) # cutted edge bottom
vol2 = (volTetra(self.gridN, A, F, B, C) + # cutted edge top
volTetra(self.gridN, A, E, F, H) + # cutted edge top
volTetra(self.gridN, A, H, F, C) + # middle
volTetra(self.gridN, C, H, D, A) + # cutted edge bottom
volTetra(self.gridN, C, G, H, F)) # cutted edge bottom
self._vol = (vol1 + vol2)/2
return self._vol
return locals()
_vol = None
vol = property(**vol())
def area():
doc = "Face areas."
def fget(self):
if(self._area is None or self._normals is None):
# Compute areas of cell faces
if(self.dim == 2):
xy = self.gridN
A, B = indexCube('AB', self.n+1, np.array([self.nNx, self.nCy]))
edge1 = xy[B, :] - xy[A, :]
normal1 = np.c_[edge1[:, 1], -edge1[:, 0]]
area1 = length2D(edge1)
A, D = indexCube('AD', self.n+1, np.array([self.nCx, self.nNy]))
# Note that we are doing A-D to make sure the normal points the right way.
# Think about it. Look at the picture. Normal points towards C iff you do this.
edge2 = xy[A, :] - xy[D, :]
normal2 = np.c_[edge2[:, 1], -edge2[:, 0]]
area2 = length2D(edge2)
self._area = np.r_[mkvc(area1), mkvc(area2)]
self._normals = [normalize2D(normal1), normalize2D(normal2)]
elif(self.dim == 3):
A, E, F, B = indexCube('AEFB', self.n+1, np.array([self.nNx, self.nCy, self.nCz]))
normal1, area1 = faceInfo(self.gridN, A, E, F, B, average=False, normalizeNormals=False)
A, D, H, E = indexCube('ADHE', self.n+1, np.array([self.nCx, self.nNy, self.nCz]))
normal2, area2 = faceInfo(self.gridN, A, D, H, E, average=False, normalizeNormals=False)
A, B, C, D = indexCube('ABCD', self.n+1, np.array([self.nCx, self.nCy, self.nNz]))
normal3, area3 = faceInfo(self.gridN, A, B, C, D, average=False, normalizeNormals=False)
self._area = np.r_[mkvc(area1), mkvc(area2), mkvc(area3)]
self._normals = [normal1, normal2, normal3]
return self._area
return locals()
_area = None
area = property(**area())
def normals():
doc = """Face normals: calling this will average
the computed normals so that there is one
per face. This is especially relevant in
3D, as there are up to 4 different normals
for each face that will be different.
To reshape the normals into a matrix and get the y component::
NyX, NyY, NyZ = M.r(M.normals, 'F', 'Fy', 'M')
"""
def fget(self):
if(self._normals is None):
self.area # calling .area will create the face normals
if self.dim == 2:
return normalize2D(np.r_[self._normals[0], self._normals[1]])
elif self.dim == 3:
normal1 = (self._normals[0][0] + self._normals[0][1] + self._normals[0][2] + self._normals[0][3])/4
normal2 = (self._normals[1][0] + self._normals[1][1] + self._normals[1][2] + self._normals[1][3])/4
normal3 = (self._normals[2][0] + self._normals[2][1] + self._normals[2][2] + self._normals[2][3])/4
return normalize3D(np.r_[normal1, normal2, normal3])
return locals()
_normals = None
normals = property(**normals())
def edge():
doc = "Edge legnths."
def fget(self):
if(self._edge is None or self._tangents is None):
if(self.dim == 2):
xy = self.gridN
A, D = indexCube('AD', self.n+1, np.array([self.nCx, self.nNy]))
edge1 = xy[D, :] - xy[A, :]
A, B = indexCube('AB', self.n+1, np.array([self.nNx, self.nCy]))
edge2 = xy[B, :] - xy[A, :]
self._edge = np.r_[mkvc(length2D(edge1)), mkvc(length2D(edge2))]
self._tangents = np.r_[edge1, edge2]/np.c_[self._edge, self._edge]
elif(self.dim == 3):
xyz = self.gridN
A, D = indexCube('AD', self.n+1, np.array([self.nCx, self.nNy, self.nNz]))
edge1 = xyz[D, :] - xyz[A, :]
A, B = indexCube('AB', self.n+1, np.array([self.nNx, self.nCy, self.nNz]))
edge2 = xyz[B, :] - xyz[A, :]
A, E = indexCube('AE', self.n+1, np.array([self.nNx, self.nNy, self.nCz]))
edge3 = xyz[E, :] - xyz[A, :]
self._edge = np.r_[mkvc(length3D(edge1)), mkvc(length3D(edge2)), mkvc(length3D(edge3))]
self._tangents = np.r_[edge1, edge2, edge3]/np.c_[self._edge, self._edge, self._edge]
return self._edge
return locals()
_edge = None
edge = property(**edge())
def tangents():
doc = "Edge tangents."
def fget(self):
if(self._tangents is None):
self.edge # calling .edge will create the tangents
return self._tangents
return locals()
_tangents = None
tangents = property(**tangents())
if __name__ == '__main__':
nc = 5
h1 = np.cumsum(np.r_[0, np.ones(nc)/(nc)])
nc = 7
h2 = np.cumsum(np.r_[0, np.ones(nc)/(nc)])
h3 = np.cumsum(np.r_[0, np.ones(nc)/(nc)])
dee3 = True
if dee3:
X, Y, Z = ndgrid(h1, h2, h3, vector=False)
M = LogicallyOrthogonalMesh([X, Y, Z])
else:
X, Y = ndgrid(h1, h2, vector=False)
M = LogicallyOrthogonalMesh([X, Y])
print M.r(M.normals, 'F', 'Fx', 'V')
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import numpy as np
import matplotlib.pyplot as plt
import matplotlib
from mpl_toolkits.mplot3d import Axes3D
from SimPEG.utils import mkvc
class LomView(object):
"""
Provides viewing functions for LogicallyOrthogonalMesh
This class is inherited by LogicallyOrthogonalMesh
"""
def __init__(self):
pass
def plotGrid(self, length=0.05):
"""Plot the nodal, cell-centered and staggered grids for 1,2 and 3 dimensions.
.. plot:: examples/mesh/plot_LogicallyOrthogonalMesh.py
"""
NN = self.r(self.gridN, 'N', 'N', 'M')
if self.dim == 2:
fig = plt.figure(2)
fig.clf()
ax = plt.subplot(111)
X1 = np.c_[mkvc(NN[0][:-1, :]), mkvc(NN[0][1:, :]), mkvc(NN[0][:-1, :])*np.nan].flatten()
Y1 = np.c_[mkvc(NN[1][:-1, :]), mkvc(NN[1][1:, :]), mkvc(NN[1][:-1, :])*np.nan].flatten()
X2 = np.c_[mkvc(NN[0][:, :-1]), mkvc(NN[0][:, 1:]), mkvc(NN[0][:, :-1])*np.nan].flatten()
Y2 = np.c_[mkvc(NN[1][:, :-1]), mkvc(NN[1][:, 1:]), mkvc(NN[1][:, :-1])*np.nan].flatten()
X = np.r_[X1, X2]
Y = np.r_[Y1, Y2]
plt.plot(X, Y)
plt.hold(True)
Nx = self.r(self.normals, 'F', 'Fx', 'V')
Ny = self.r(self.normals, 'F', 'Fy', 'V')
Tx = self.r(self.tangents, 'E', 'Ex', 'V')
Ty = self.r(self.tangents, 'E', 'Ey', 'V')
plt.plot(self.gridN[:, 0], self.gridN[:, 1], 'bo')
nX = np.c_[self.gridFx[:, 0], self.gridFx[:, 0] + Nx[0]*length, self.gridFx[:, 0]*np.nan].flatten()
nY = np.c_[self.gridFx[:, 1], self.gridFx[:, 1] + Nx[1]*length, self.gridFx[:, 1]*np.nan].flatten()
plt.plot(self.gridFx[:, 0], self.gridFx[:, 1], 'rs')
plt.plot(nX, nY, 'r-')
nX = np.c_[self.gridFy[:, 0], self.gridFy[:, 0] + Ny[0]*length, self.gridFy[:, 0]*np.nan].flatten()
nY = np.c_[self.gridFy[:, 1], self.gridFy[:, 1] + Ny[1]*length, self.gridFy[:, 1]*np.nan].flatten()
#plt.plot(self.gridFy[:, 0], self.gridFy[:, 1], 'gs')
plt.plot(nX, nY, 'g-')
tX = np.c_[self.gridEx[:, 0], self.gridEx[:, 0] + Tx[0]*length, self.gridEx[:, 0]*np.nan].flatten()
tY = np.c_[self.gridEx[:, 1], self.gridEx[:, 1] + Tx[1]*length, self.gridEx[:, 1]*np.nan].flatten()
plt.plot(self.gridEx[:, 0], self.gridEx[:, 1], 'r^')
plt.plot(tX, tY, 'r-')
nX = np.c_[self.gridEy[:, 0], self.gridEy[:, 0] + Ty[0]*length, self.gridEy[:, 0]*np.nan].flatten()
nY = np.c_[self.gridEy[:, 1], self.gridEy[:, 1] + Ty[1]*length, self.gridEy[:, 1]*np.nan].flatten()
#plt.plot(self.gridEy[:, 0], self.gridEy[:, 1], 'g^')
plt.plot(nX, nY, 'g-')
plt.axis('equal')
elif self.dim == 3:
fig = plt.figure(3)
fig.clf()
ax = fig.add_subplot(111, projection='3d')
X1 = np.c_[mkvc(NN[0][:-1, :, :]), mkvc(NN[0][1:, :, :]), mkvc(NN[0][:-1, :, :])*np.nan].flatten()
Y1 = np.c_[mkvc(NN[1][:-1, :, :]), mkvc(NN[1][1:, :, :]), mkvc(NN[1][:-1, :, :])*np.nan].flatten()
Z1 = np.c_[mkvc(NN[2][:-1, :, :]), mkvc(NN[2][1:, :, :]), mkvc(NN[2][:-1, :, :])*np.nan].flatten()
X2 = np.c_[mkvc(NN[0][:, :-1, :]), mkvc(NN[0][:, 1:, :]), mkvc(NN[0][:, :-1, :])*np.nan].flatten()
Y2 = np.c_[mkvc(NN[1][:, :-1, :]), mkvc(NN[1][:, 1:, :]), mkvc(NN[1][:, :-1, :])*np.nan].flatten()
Z2 = np.c_[mkvc(NN[2][:, :-1, :]), mkvc(NN[2][:, 1:, :]), mkvc(NN[2][:, :-1, :])*np.nan].flatten()
X3 = np.c_[mkvc(NN[0][:, :, :-1]), mkvc(NN[0][:, :, 1:]), mkvc(NN[0][:, :, :-1])*np.nan].flatten()
Y3 = np.c_[mkvc(NN[1][:, :, :-1]), mkvc(NN[1][:, :, 1:]), mkvc(NN[1][:, :, :-1])*np.nan].flatten()
Z3 = np.c_[mkvc(NN[2][:, :, :-1]), mkvc(NN[2][:, :, 1:]), mkvc(NN[2][:, :, :-1])*np.nan].flatten()
X = np.r_[X1, X2, X3]
Y = np.r_[Y1, Y2, Y3]
Z = np.r_[Z1, Z2, Z3]
plt.plot(X, Y, 'b', zs=Z)
ax.set_zlabel('x3')
ax.grid(True)
ax.hold(False)
ax.set_xlabel('x1')
ax.set_ylabel('x2')
fig.show()
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import numpy as np
from BaseMesh import BaseMesh
from TensorView import TensorView
from DiffOperators import DiffOperators
from InnerProducts import InnerProducts
from SimPEG.utils import ndgrid, mkvc
class TensorMesh(BaseMesh, TensorView, DiffOperators, InnerProducts):
"""
TensorMesh is a mesh class that deals with tensor product meshes.
Any Mesh that has a constant width along the entire axis
such that it can defined by a single width vector, called 'h'.
::
hx = np.array([1,1,1])
hy = np.array([1,2])
hz = np.array([1,1,1,1])
mesh = TensorMesh([hx, hy, hz])
Example of a padded tensor mesh:
.. plot:: examples/mesh/plot_TensorMesh.py
"""
_meshType = 'TENSOR'
def __init__(self, h, x0=None):
super(TensorMesh, self).__init__(np.array([x.size for x in h]), x0)
assert len(h) == len(self.x0), "Dimension mismatch. x0 != len(h)"
for i, h_i in enumerate(h):
assert type(h_i) == np.ndarray, ("h[%i] is not a numpy array." % i)
assert len(h_i.shape) == 1, ("h[%i] must be a 1D numpy array." % i)
# Ensure h contains 1D vectors
self._h = [mkvc(x) for x in h]
def __str__(self):
outStr = ' ---- {0:d}-D TensorMesh ---- '.format(self.dim)
def printH(hx, outStr=''):
i = -1
while True:
i = i + 1
if i > hx.size:
break
elif i == hx.size:
break
h = hx[i]
n = 1
for j in range(i+1, hx.size):
if hx[j] == h:
n = n + 1
i = i + 1
else:
break
if n == 1:
outStr = outStr + ' {0:.2f},'.format(h)
else:
outStr = outStr + ' {0:d}*{1:.2f},'.format(n,h)
return outStr[:-1]
if self.dim == 1:
outStr = outStr + '\n x0: {0:.2f}'.format(self.x0[0])
outStr = outStr + '\n nCx: {0:d}'.format(self.nCx)
outStr = outStr + printH(self.hx, outStr='\n hx:')
pass
elif self.dim == 2:
outStr = outStr + '\n x0: {0:.2f}'.format(self.x0[0])
outStr = outStr + '\n y0: {0:.2f}'.format(self.x0[1])
outStr = outStr + '\n nCx: {0:d}'.format(self.nCx)
outStr = outStr + '\n nCy: {0:d}'.format(self.nCy)
outStr = outStr + printH(self.hx, outStr='\n hx:')
outStr = outStr + printH(self.hy, outStr='\n hy:')
elif self.dim == 3:
outStr = outStr + '\n x0: {0:.2f}'.format(self.x0[0])
outStr = outStr + '\n y0: {0:.2f}'.format(self.x0[1])
outStr = outStr + '\n z0: {0:.2f}'.format(self.x0[2])
outStr = outStr + '\n nCx: {0:d}'.format(self.nCx)
outStr = outStr + '\n nCy: {0:d}'.format(self.nCy)
outStr = outStr + '\n nCz: {0:d}'.format(self.nCz)
outStr = outStr + printH(self.hx, outStr='\n hx:')
outStr = outStr + printH(self.hy, outStr='\n hy:')
outStr = outStr + printH(self.hz, outStr='\n hz:')
return outStr
def h():
doc = "h is a list containing the cell widths of the tensor mesh in each dimension."
fget = lambda self: self._h
return locals()
h = property(**h())
def hx():
doc = "Width of cells in the x direction"
fget = lambda self: self._h[0]
return locals()
hx = property(**hx())
def hy():
doc = "Width of cells in the y direction"
fget = lambda self: None if self.dim < 2 else self._h[1]
return locals()
hy = property(**hy())
def hz():
doc = "Width of cells in the z direction"
fget = lambda self: None if self.dim < 3 else self._h[2]
return locals()
hz = property(**hz())
def vectorNx():
doc = "Nodal grid vector (1D) in the x direction."
fget = lambda self: np.r_[0., self.hx.cumsum()] + self.x0[0]
return locals()
vectorNx = property(**vectorNx())
def vectorNy():
doc = "Nodal grid vector (1D) in the y direction."
fget = lambda self: None if self.dim < 2 else np.r_[0., self.hy.cumsum()] + self.x0[1]
return locals()
vectorNy = property(**vectorNy())
def vectorNz():
doc = "Nodal grid vector (1D) in the z direction."
fget = lambda self: None if self.dim < 3 else np.r_[0., self.hz.cumsum()] + self.x0[2]
return locals()
vectorNz = property(**vectorNz())
def vectorCCx():
doc = "Cell-centered grid vector (1D) in the x direction."
fget = lambda self: np.r_[0, self.hx[:-1].cumsum()] + self.hx*0.5 + self.x0[0]
return locals()
vectorCCx = property(**vectorCCx())
def vectorCCy():
doc = "Cell-centered grid vector (1D) in the y direction."
fget = lambda self: None if self.dim < 2 else np.r_[0, self.hy[:-1].cumsum()] + self.hy*0.5 + self.x0[1]
return locals()
vectorCCy = property(**vectorCCy())
def vectorCCz():
doc = "Cell-centered grid vector (1D) in the z direction."
fget = lambda self: None if self.dim < 3 else np.r_[0, self.hz[:-1].cumsum()] + self.hz*0.5 + self.x0[2]
return locals()
vectorCCz = property(**vectorCCz())
def gridCC():
doc = "Cell-centered grid."
def fget(self):
if self._gridCC is None:
self._gridCC = ndgrid([x for x in [self.vectorCCx, self.vectorCCy, self.vectorCCz] if not x is None])
return self._gridCC
return locals()
_gridCC = None # Store grid by default
gridCC = property(**gridCC())
def gridN():
doc = "Nodal grid."
def fget(self):
if self._gridN is None:
self._gridN = ndgrid([x for x in [self.vectorNx, self.vectorNy, self.vectorNz] if not x is None])
return self._gridN
return locals()
_gridN = None # Store grid by default
gridN = property(**gridN())
def gridFx():
doc = "Face staggered grid in the x direction."
def fget(self):
if self._gridFx is None:
self._gridFx = ndgrid([x for x in [self.vectorNx, self.vectorCCy, self.vectorCCz] if not x is None])
return self._gridFx
return locals()
_gridFx = None # Store grid by default
gridFx = property(**gridFx())
def gridFy():
doc = "Face staggered grid in the y direction."
def fget(self):
if self._gridFy is None and self.dim > 1:
self._gridFy = ndgrid([x for x in [self.vectorCCx, self.vectorNy, self.vectorCCz] if not x is None])
return self._gridFy
return locals()
_gridFy = None # Store grid by default
gridFy = property(**gridFy())
def gridFz():
doc = "Face staggered grid in the z direction."
def fget(self):
if self._gridFz is None and self.dim > 2:
self._gridFz = ndgrid([x for x in [self.vectorCCx, self.vectorCCy, self.vectorNz] if not x is None])
return self._gridFz
return locals()
_gridFz = None # Store grid by default
gridFz = property(**gridFz())
def gridEx():
doc = "Edge staggered grid in the x direction."
def fget(self):
if self._gridEx is None:
self._gridEx = ndgrid([x for x in [self.vectorCCx, self.vectorNy, self.vectorNz] if not x is None])
return self._gridEx
return locals()
_gridEx = None # Store grid by default
gridEx = property(**gridEx())
def gridEy():
doc = "Edge staggered grid in the y direction."
def fget(self):
if self._gridEy is None and self.dim > 1:
self._gridEy = ndgrid([x for x in [self.vectorNx, self.vectorCCy, self.vectorNz] if not x is None])
return self._gridEy
return locals()
_gridEy = None # Store grid by default
gridEy = property(**gridEy())
def gridEz():
doc = "Edge staggered grid in the z direction."
def fget(self):
if self._gridEz is None and self.dim > 2:
self._gridEz = ndgrid([x for x in [self.vectorNx, self.vectorNy, self.vectorCCz] if not x is None])
return self._gridEz
return locals()
_gridEz = None # Store grid by default
gridEz = property(**gridEz())
# --------------- Geometries ---------------------
def vol():
doc = "Construct cell volumes of the 3D model as 1d array."
def fget(self):
if(self._vol is None):
vh = self.h
# Compute cell volumes
if(self.dim == 1):
self._vol = mkvc(vh[0])
elif(self.dim == 2):
# Cell sizes in each direction
self._vol = mkvc(np.outer(vh[0], vh[1]))
elif(self.dim == 3):
# Cell sizes in each direction
self._vol = mkvc(np.outer(mkvc(np.outer(vh[0], vh[1])), vh[2]))
return self._vol
return locals()
_vol = None
vol = property(**vol())
def area():
doc = "Construct face areas of the 3D model as 1d array."
def fget(self):
if(self._area is None):
# Ensure that we are working with column vectors
vh = self.h
# The number of cell centers in each direction
n = self.n
# Compute areas of cell faces
if(self.dim == 1):
self._area = np.ones(n[0]+1)
elif(self.dim == 2):
area1 = np.outer(np.ones(n[0]+1), vh[1])
area2 = np.outer(vh[0], np.ones(n[1]+1))
self._area = np.r_[mkvc(area1), mkvc(area2)]
elif(self.dim == 3):
area1 = np.outer(np.ones(n[0]+1), mkvc(np.outer(vh[1], vh[2])))
area2 = np.outer(vh[0], mkvc(np.outer(np.ones(n[1]+1), vh[2])))
area3 = np.outer(vh[0], mkvc(np.outer(vh[1], np.ones(n[2]+1))))
self._area = np.r_[mkvc(area1), mkvc(area2), mkvc(area3)]
return self._area
return locals()
_area = None
area = property(**area())
def edge():
doc = "Construct edge legnths of the 3D model as 1d array."
def fget(self):
if(self._edge is None):
# Ensure that we are working with column vectors
vh = self.h
# The number of cell centers in each direction
n = self.n
# Compute edge lengths
if(self.dim == 1):
self._edge = mkvc(vh[0])
elif(self.dim == 2):
l1 = np.outer(vh[0], np.ones(n[1]+1))
l2 = np.outer(np.ones(n[0]+1), vh[1])
self._edge = np.r_[mkvc(l1), mkvc(l2)]
elif(self.dim == 3):
l1 = np.outer(vh[0], mkvc(np.outer(np.ones(n[1]+1), np.ones(n[2]+1))))
l2 = np.outer(np.ones(n[0]+1), mkvc(np.outer(vh[1], np.ones(n[2]+1))))
l3 = np.outer(np.ones(n[0]+1), mkvc(np.outer(np.ones(n[1]+1), vh[2])))
self._edge = np.r_[mkvc(l1), mkvc(l2), mkvc(l3)]
return self._edge
return locals()
_edge = None
edge = property(**edge())
if __name__ == '__main__':
print('Welcome to tensor mesh!')
testDim = 1
h1 = 0.3*np.ones(7)
h1[0] = 0.5
h1[-1] = 0.6
h2 = .5 * np.ones(4)
h3 = .4 * np.ones(6)
h = [h1, h2, h3]
h = h[:testDim]
M = TensorMesh(h)
xn = M.plotGrid()
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import numpy as np
import matplotlib.pyplot as plt
import matplotlib
from mpl_toolkits.mplot3d import Axes3D
from SimPEG.utils import mkvc
class TensorView(object):
"""
Provides viewing functions for TensorMesh
This class is inherited by TensorMesh
"""
def __init__(self):
pass
def plotImage(self, I, imageType='CC', figNum=1,ax=None,direction='z',numbering=True,annotationColor='w',showIt=False):
"""
Mesh.plotImage(I)
Plots scalar fields on the given mesh.
Input:
:param numpy.array I: scalar field
Optional Input:
:param str imageType: type of image ('CC','N','F','Fx','Fy','Fz','E','Ex','Ey','Ez') or combinations, e.g. ExEy or FxFz
:param int figNum: number of figure to plot to
:param matplotlib.axes.Axes ax: axis to plot to
:param str direction: slice dimensions, 3D only ('x', 'y', 'z')
:param bool numbering: show numbering of slices, 3D only
:param str annotationColor: color of annotation, e.g. 'w', 'k', 'b'
:param bool showIt: call plt.show()
.. plot:: examples/mesh/plot_image_2D.py
:include-source:
.. plot:: examples/mesh/plot_image_3D.py
:include-source:
"""
assert type(I) == np.ndarray, "I must be a numpy array"
assert type(numbering) == bool, "numbering must be a bool"
assert direction in ["x", "y","z"], "direction must be either x,y, or z"
if imageType == 'CC':
assert I.size == self.nC, "Incorrect dimensions for CC."
elif imageType == 'N':
assert I.size == self.nN, "Incorrect dimensions for N."
elif imageType == 'Fx':
if I.size != np.prod(self.nFx): I, fy, fz = self.r(I,'F','F','M')
elif imageType == 'Fy':
if I.size != np.prod(self.nFy): fx, I, fz = self.r(I,'F','F','M')
elif imageType == 'Fz':
if I.size != np.prod(self.nFz): fx, fy, I = self.r(I,'F','F','M')
elif imageType == 'Ex':
if I.size != np.prod(self.nEx): I, ey, ez = self.r(I,'E','E','M')
elif imageType == 'Ey':
if I.size != np.prod(self.nEy): ex, I, ez = self.r(I,'E','E','M')
elif imageType == 'Ez':
if I.size != np.prod(self.nEz): ex, ey, I = self.r(I,'E','E','M')
elif imageType[0] == 'E':
plotAll = len(imageType) == 1
options = {"direction":direction,"numbering":numbering,"annotationColor":annotationColor,"showIt":showIt}
fig = plt.figure(figNum)
# Determine the subplot number: 131, 121
numPlots = 130 if plotAll else len(imageType)/2*10+100
pltNum = 1
ex, ey, ez = self.r(I,'E','E','M')
if plotAll or 'Ex' in imageType:
ax_x = plt.subplot(numPlots+pltNum)
self.plotImage(ex, imageType='Ex', ax=ax_x, **options)
pltNum +=1
if plotAll or 'Ey' in imageType:
ax_y = plt.subplot(numPlots+pltNum)
self.plotImage(ey, imageType='Ey', ax=ax_y, **options)
pltNum +=1
if plotAll or 'Ez' in imageType:
ax_z = plt.subplot(numPlots+pltNum)
self.plotImage(ez, imageType='Ez', ax=ax_z, **options)
pltNum +=1
return
elif imageType[0] == 'F':
plotAll = len(imageType) == 1
options = {"direction":direction,"numbering":numbering,"annotationColor":annotationColor,"showIt":showIt}
fig = plt.figure(figNum)
# Determine the subplot number: 131, 121
numPlots = 130 if plotAll else len(imageType)/2*10+100
pltNum = 1
fx, fy, fz = self.r(I,'F','F','M')
if plotAll or 'Fx' in imageType:
ax_x = plt.subplot(numPlots+pltNum)
self.plotImage(fx, imageType='Fx', ax=ax_x, **options)
pltNum +=1
if plotAll or 'Fy' in imageType:
ax_y = plt.subplot(numPlots+pltNum)
self.plotImage(fy, imageType='Fy', ax=ax_y, **options)
pltNum +=1
if plotAll or 'Fz' in imageType:
ax_z = plt.subplot(numPlots+pltNum)
self.plotImage(fz, imageType='Fz', ax=ax_z, **options)
pltNum +=1
return
else:
raise Exception("imageType must be 'CC', 'N','Fx','Fy','Fz','Ex','Ey','Ez'")
if ax is None:
fig = plt.figure(figNum)
fig.clf()
ax = plt.subplot(111)
else:
assert isinstance(ax,matplotlib.axes.Axes), "ax must be an Axes!"
fig = ax.figure
if self.dim == 1:
if imageType == 'CC':
ph = ax.plot(self.vectorCCx, I, '-ro')
elif imageType == 'N':
ph = ax.plot(self.vectorNx, I, '-bs')
ax.set_xlabel("x")
ax.axis('tight')
elif self.dim == 2:
if imageType == 'CC':
C = I[:].reshape(self.n, order='F')
elif imageType == 'N':
C = I[:].reshape(self.n+1, order='F')
C = 0.25*(C[:-1, :-1] + C[1:, :-1] + C[:-1, 1:] + C[1:, 1:])
elif imageType == 'Fx':
C = I[:].reshape(self.nFx, order='F')
C = 0.5*(C[:-1, :] + C[1:, :] )
elif imageType == 'Fy':
C = I[:].reshape(self.nFy, order='F')
C = 0.5*(C[:, :-1] + C[:, 1:] )
elif imageType == 'Ex':
C = I[:].reshape(self.nEx, order='F')
C = 0.5*(C[:,:-1] + C[:,1:] )
elif imageType == 'Ey':
C = I[:].reshape(self.nEy, order='F')
C = 0.5*(C[:-1,:] + C[1:,:] )
ph = ax.pcolormesh(self.vectorNx, self.vectorNy, C.T)
ax.axis('tight')
ax.set_xlabel("x")
ax.set_ylabel("y")
elif self.dim == 3:
if direction == 'z':
# get copy of image and average to cell-centres is necessary
if imageType == 'CC':
Ic = I[:].reshape(self.n, order='F')
elif imageType == 'N':
Ic = I[:].reshape(self.n+1, order='F')
Ic = .125*(Ic[:-1,:-1,:-1]+Ic[1:,:-1,:-1] + Ic[:-1,1:,:-1]+ Ic[1:,1:,:-1]+ Ic[:-1,:-1,1:]+Ic[1:,:-1,1:] + Ic[:-1,1:,1:]+ Ic[1:,1:,1:] )
elif imageType == 'Fx':
Ic = I[:].reshape(self.nFx, order='F')
Ic = .5*(Ic[:-1,:,:]+Ic[1:,:,:])
elif imageType == 'Fy':
Ic = I[:].reshape(self.nFy, order='F')
Ic = .5*(Ic[:,:-1,:]+Ic[:,1:,:])
elif imageType == 'Fz':
Ic = I[:].reshape(self.nFz, order='F')
Ic = .5*(Ic[:,:,:-1]+Ic[:,:,1:])
elif imageType == 'Ex':
Ic = I[:].reshape(self.nEx, order='F')
Ic = .25*(Ic[:,:-1,:-1]+Ic[:,1:,:-1]+Ic[:,:-1,1:]+Ic[:,1:,:1])
elif imageType == 'Ey':
Ic = I[:].reshape(self.nEy, order='F')
Ic = .25*(Ic[:-1,:,:-1]+Ic[1:,:,:-1]+Ic[:-1,:,1:]+Ic[1:,:,:1])
elif imageType == 'Ez':
Ic = I[:].reshape(self.nEz, order='F')
Ic = .25*(Ic[:-1,:-1,:]+Ic[1:,:-1,:]+Ic[:-1,1:,:]+Ic[1:,:1,:])
# determine number oE slices in x and y dimension
nX = np.ceil(np.sqrt(self.nCz))
nY = np.ceil(self.nCz/nX)
# allocate space for montage
nCx = self.nCx
nCy = self.nCy
C = np.zeros((nX*nCx,nY*nCy))
for iy in range(int(nY)):
for ix in range(int(nX)):
iz = ix + iy*nX
if iz < self.nCz:
C[ix*nCx:(ix+1)*nCx, iy*nCy:(iy+1)*nCy] = Ic[:, :, iz]
else:
C[ix*nCx:(ix+1)*nCx, iy*nCy:(iy+1)*nCy] = np.nan
C = np.ma.masked_where(np.isnan(C), C)
xx = np.r_[0, np.cumsum(np.kron(np.ones((nX, 1)), self.hx).ravel())]
yy = np.r_[0, np.cumsum(np.kron(np.ones((nY, 1)), self.hy).ravel())]
# Plot the mesh
ph = ax.pcolormesh(xx, yy, C.T)
# Plot the lines
gx = np.arange(nX+1)*(self.vectorNx[-1]-self.x0[0])
gy = np.arange(nY+1)*(self.vectorNy[-1]-self.x0[1])
# Repeat and seperate with NaN
gxX = np.c_[gx, gx, gx+np.nan].ravel()
gxY = np.kron(np.ones((nX+1, 1)), np.array([0, sum(self.hy)*nY, np.nan])).ravel()
gyX = np.kron(np.ones((nY+1, 1)), np.array([0, sum(self.hx)*nX, np.nan])).ravel()
gyY = np.c_[gy, gy, gy+np.nan].ravel()
ax.plot(gxX, gxY, annotationColor+'-', linewidth=2)
ax.plot(gyX, gyY, annotationColor+'-', linewidth=2)
ax.axis('tight')
if numbering:
pad = np.sum(self.hx)*0.04
for iy in range(int(nY)):
for ix in range(int(nX)):
iz = ix + iy*nX
if iz < self.nCz:
ax.text((ix+1)*(self.vectorNx[-1]-self.x0[0])-pad,(iy)*(self.vectorNy[-1]-self.x0[1])+pad,
'#%i'%iz,color=annotationColor,verticalalignment='bottom',horizontalalignment='right',size='x-large')
ax.set_title(imageType)
if showIt: plt.show()
return ph
def plotGrid(self, nodes=False, faces=False, centers=False, edges=False, lines=True, showIt=False):
"""Plot the nodal, cell-centered and staggered grids for 1,2 and 3 dimensions.
:param bool nodes: plot nodes
:param bool faces: plot faces
:param bool centers: plot centers
:param bool edges: plot edges
:param bool lines: plot lines connecting nodes
:param bool showIt: call plt.show()
.. plot:: examples/mesh/plot_grid_2D.py
:include-source:
.. plot:: examples/mesh/plot_grid_3D.py
:include-source:
"""
if self.dim == 1:
fig = plt.figure(1)
fig.clf()
ax = plt.subplot(111)
xn = self.gridN
xc = self.gridCC
ax.hold(True)
ax.plot(xn, np.ones(np.shape(xn)), 'bs')
ax.plot(xc, np.ones(np.shape(xc)), 'ro')
ax.plot(xn, np.ones(np.shape(xn)), 'k--')
ax.grid(True)
ax.hold(False)
ax.set_xlabel('x1')
if showIt: plt.show()
elif self.dim == 2:
fig = plt.figure(2)
fig.clf()
ax = plt.subplot(111)
xn = self.gridN
xc = self.gridCC
xs1 = self.gridFx
xs2 = self.gridFy
ax.hold(True)
if nodes: ax.plot(xn[:, 0], xn[:, 1], 'bs')
if centers: ax.plot(xc[:, 0], xc[:, 1], 'ro')
if faces:
ax.plot(xs1[:, 0], xs1[:, 1], 'g>')
ax.plot(xs2[:, 0], xs2[:, 1], 'g^')
# Plot the grid lines
if lines:
NN = self.r(self.gridN, 'N', 'N', 'M')
X1 = np.c_[mkvc(NN[0][0, :]), mkvc(NN[0][self.nCx, :]), mkvc(NN[0][0, :])*np.nan].flatten()
Y1 = np.c_[mkvc(NN[1][0, :]), mkvc(NN[1][self.nCx, :]), mkvc(NN[1][0, :])*np.nan].flatten()
X2 = np.c_[mkvc(NN[0][:, 0]), mkvc(NN[0][:, self.nCy]), mkvc(NN[0][:, 0])*np.nan].flatten()
Y2 = np.c_[mkvc(NN[1][:, 0]), mkvc(NN[1][:, self.nCy]), mkvc(NN[1][:, 0])*np.nan].flatten()
X = np.r_[X1, X2]
Y = np.r_[Y1, Y2]
plt.plot(X, Y)
ax.grid(True)
ax.hold(False)
ax.set_xlabel('x1')
ax.set_ylabel('x2')
if showIt: plt.show()
elif self.dim == 3:
fig = plt.figure(3)
fig.clf()
ax = fig.add_subplot(111, projection='3d')
xn = self.gridN
xc = self.gridCC
xfs1 = self.gridFx
xfs2 = self.gridFy
xfs3 = self.gridFz
xes1 = self.gridEx
xes2 = self.gridEy
xes3 = self.gridEz
ax.hold(True)
if nodes: ax.plot(xn[:, 0], xn[:, 1], 'bs', zs=xn[:, 2])
if centers: ax.plot(xc[:, 0], xc[:, 1], 'ro', zs=xc[:, 2])
if faces:
ax.plot(xfs1[:, 0], xfs1[:, 1], 'g>', zs=xfs1[:, 2])
ax.plot(xfs2[:, 0], xfs2[:, 1], 'g<', zs=xfs2[:, 2])
ax.plot(xfs3[:, 0], xfs3[:, 1], 'g^', zs=xfs3[:, 2])
if edges:
ax.plot(xes1[:, 0], xes1[:, 1], 'k>', zs=xes1[:, 2])
ax.plot(xes2[:, 0], xes2[:, 1], 'k<', zs=xes2[:, 2])
ax.plot(xes3[:, 0], xes3[:, 1], 'k^', zs=xes3[:, 2])
# Plot the grid lines
if lines:
NN = self.r(self.gridN, 'N', 'N', 'M')
X1 = np.c_[mkvc(NN[0][0, :, :]), mkvc(NN[0][self.nCx, :, :]), mkvc(NN[0][0, :, :])*np.nan].flatten()
Y1 = np.c_[mkvc(NN[1][0, :, :]), mkvc(NN[1][self.nCx, :, :]), mkvc(NN[1][0, :, :])*np.nan].flatten()
Z1 = np.c_[mkvc(NN[2][0, :, :]), mkvc(NN[2][self.nCx, :, :]), mkvc(NN[2][0, :, :])*np.nan].flatten()
X2 = np.c_[mkvc(NN[0][:, 0, :]), mkvc(NN[0][:, self.nCy, :]), mkvc(NN[0][:, 0, :])*np.nan].flatten()
Y2 = np.c_[mkvc(NN[1][:, 0, :]), mkvc(NN[1][:, self.nCy, :]), mkvc(NN[1][:, 0, :])*np.nan].flatten()
Z2 = np.c_[mkvc(NN[2][:, 0, :]), mkvc(NN[2][:, self.nCy, :]), mkvc(NN[2][:, 0, :])*np.nan].flatten()
X3 = np.c_[mkvc(NN[0][:, :, 0]), mkvc(NN[0][:, :, self.nCz]), mkvc(NN[0][:, :, 0])*np.nan].flatten()
Y3 = np.c_[mkvc(NN[1][:, :, 0]), mkvc(NN[1][:, :, self.nCz]), mkvc(NN[1][:, :, 0])*np.nan].flatten()
Z3 = np.c_[mkvc(NN[2][:, :, 0]), mkvc(NN[2][:, :, self.nCz]), mkvc(NN[2][:, :, 0])*np.nan].flatten()
X = np.r_[X1, X2, X3]
Y = np.r_[Y1, Y2, Y3]
Z = np.r_[Z1, Z2, Z3]
plt.plot(X, Y, 'b-', zs=Z)
ax.grid(True)
ax.hold(False)
ax.set_xlabel('x1')
ax.set_ylabel('x2')
ax.set_zlabel('x3')
if showIt: plt.show()
+8
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@@ -0,0 +1,8 @@
from TensorMesh import TensorMesh
from LogicallyOrthogonalMesh import LogicallyOrthogonalMesh
from BaseMesh import BaseMesh
from TensorView import TensorView
from LomView import LomView
from InnerProducts import InnerProducts
from DiffOperators import DiffOperators