mirror of
https://github.com/wassname/simpeg.git
synced 2026-07-14 11:18:18 +08:00
combine edge inner products 2D and 3D
This commit is contained in:
+101
-125
@@ -90,17 +90,108 @@ class InnerProducts(object):
|
||||
elif self.dim == 3:
|
||||
return getFaceInnerProduct(self, mu, returnP)
|
||||
|
||||
def getEdgeInnerProduct(self, sigma=None, returnP=False):
|
||||
"""Wrapper function,
|
||||
|
||||
:py:func:`SimPEG.mesh.InnerProducts.InnerProducts.getEdgeInnerProduct`
|
||||
|
||||
:py:func:`SimPEG.mesh.InnerProducts.InnerProducts.getEdgeInnerProduct2D`
|
||||
def getEdgeInnerProduct(M, sigma=None, returnP=False):
|
||||
"""
|
||||
if self.dim == 2:
|
||||
return getEdgeInnerProduct2D(self, sigma, returnP)
|
||||
elif self.dim == 3:
|
||||
return getEdgeInnerProduct(self, sigma, returnP)
|
||||
: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.
|
||||
|
||||
**For 2D:**
|
||||
|
||||
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.
|
||||
|
||||
"""
|
||||
# We will multiply by V on each side to keep symmetry
|
||||
if M.dim == 2:
|
||||
# Square root of cell volume multiplied by 1/4
|
||||
v = np.sqrt(0.25*M.vol)
|
||||
V = sdiag(np.r_[v, v])
|
||||
eP = _getEdgePxx(M)
|
||||
P000 = V*eP('eX0', 'eY0')
|
||||
P100 = V*eP('eX0', 'eY1')
|
||||
P010 = V*eP('eX1', 'eY0')
|
||||
P110 = V*eP('eX1', 'eY1')
|
||||
elif M.dim == 3:
|
||||
# Square root of cell volume multiplied by 1/8
|
||||
v = np.sqrt(0.125*M.vol)
|
||||
V = sdiag(np.r_[v, v, v])
|
||||
eP = _getEdgePxxx(M)
|
||||
P000 = V*eP('eX0', 'eY0', 'eZ0')
|
||||
P100 = V*eP('eX0', 'eY1', 'eZ1')
|
||||
P010 = V*eP('eX1', 'eY0', 'eZ2')
|
||||
P110 = V*eP('eX1', 'eY1', 'eZ3')
|
||||
P001 = V*eP('eX2', 'eY2', 'eZ0')
|
||||
P101 = V*eP('eX2', 'eY3', 'eZ1')
|
||||
P011 = V*eP('eX3', 'eY2', 'eZ2')
|
||||
P111 = V*eP('eX3', 'eY3', 'eZ3')
|
||||
|
||||
Sigma = _makeTensor(M, sigma)
|
||||
A = P000.T*Sigma*P000 + P100.T*Sigma*P100 + P010.T*Sigma*P010 + P110.T*Sigma*P110
|
||||
P = [P000, P100, P010, P110]
|
||||
if M.dim == 3:
|
||||
A = A + P001.T*Sigma*P001 + P101.T*Sigma*P101 + P011.T*Sigma*P011 + P111.T*Sigma*P111
|
||||
P += [P001, P101, P011, P111]
|
||||
if returnP:
|
||||
return A, P
|
||||
else:
|
||||
return A
|
||||
|
||||
# ------------------------ Geometries ------------------------------
|
||||
#
|
||||
@@ -486,121 +577,6 @@ def getFaceInnerProduct2D(M, mu=None, returnP=False):
|
||||
return A
|
||||
|
||||
|
||||
def getEdgeInnerProduct(M, 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.
|
||||
"""
|
||||
# Square root of cell volume multiplied by 1/8
|
||||
v = np.sqrt(0.125*M.vol)
|
||||
V3 = sdiag(np.r_[v, v, v]) # We will multiply on each side to keep symmetry
|
||||
|
||||
Pxxx = _getEdgePxxx(M)
|
||||
P000 = V3*Pxxx('eX0', 'eY0', 'eZ0')
|
||||
P100 = V3*Pxxx('eX0', 'eY1', 'eZ1')
|
||||
P010 = V3*Pxxx('eX1', 'eY0', 'eZ2')
|
||||
P110 = V3*Pxxx('eX1', 'eY1', 'eZ3')
|
||||
P001 = V3*Pxxx('eX2', 'eY2', 'eZ0')
|
||||
P101 = V3*Pxxx('eX2', 'eY3', 'eZ1')
|
||||
P011 = V3*Pxxx('eX3', 'eY2', 'eZ2')
|
||||
P111 = V3*Pxxx('eX3', 'eY3', 'eZ3')
|
||||
|
||||
Sigma = _makeTensor(M, sigma)
|
||||
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(M, 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.
|
||||
|
||||
"""
|
||||
# Square root of cell volume multiplied by 1/4
|
||||
v = np.sqrt(0.25*M.vol)
|
||||
V2 = sdiag(np.r_[v, v]) # We will multiply on each side to keep symmetry
|
||||
|
||||
Pxx = _getEdgePxx(M)
|
||||
P00 = V2*Pxx('eX0', 'eY0')
|
||||
P10 = V2*Pxx('eX0', 'eY1')
|
||||
P01 = V2*Pxx('eX1', 'eY0')
|
||||
P11 = V2*Pxx('eX1', 'eY1')
|
||||
|
||||
Sigma = _makeTensor(M, sigma)
|
||||
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])]
|
||||
|
||||
Reference in New Issue
Block a user