Files
simpeg/simpegDC/BaseDC.py
T
2015-04-17 17:17:03 -07:00

230 lines
6.8 KiB
Python

from SimPEG import *
class DipoleSrc(Survey.BaseSrc):
"""A dipole source, locA and locB are moved to the closest cell-centers"""
current = 1
def __init__(self, locA, locB, rxList, **kwargs):
super(DipoleSrc, self).__init__((locA, locB), 'dipole', rxList, **kwargs)
self._rhsDict = {}
def getRhs(self, mesh):
if mesh not in self._rhsDict:
pts = [self.loc[0], self.loc[1]]
inds = Utils.closestPoints(mesh, pts)
q = np.zeros(mesh.nC)
q[inds] = - self.current * ( np.r_[1., -1.] / mesh.vol[inds] )
self._rhsDict[mesh] = q
return self._rhsDict[mesh]
class DipoleRx(Survey.BaseRx):
"""A dipole source, locA and locB are moved to the closest cell-centers"""
def __init__(self, locsM, locsN, **kwargs):
locs = (locsM, locsN)
assert locsM.shape == locsN.shape, 'locs must be the same shape.'
super(DipoleRx, self).__init__(locs, 'dipole', storeProjections=False, **kwargs)
@property
def nD(self):
"""Number of data in the receiver."""
return self.locs[0].shape[0]
def getP(self, mesh):
P0 = mesh.getInterpolationMat(self.locs[0], self.projGLoc)
P1 = mesh.getInterpolationMat(self.locs[1], self.projGLoc)
return P0 - P1
class SurveyDC(Survey.BaseSurvey):
"""
**SurveyDC**
Geophysical DC resistivity data.
"""
def __init__(self, srcList, **kwargs):
self.srcList = srcList
Survey.BaseSurvey.__init__(self, **kwargs)
self._rhsDict = {}
self._Ps = {}
def projectFields(self, u):
"""
Predicted data.
.. math::
d_\\text{pred} = Pu(m)
"""
P = self.getP(self.prob.mesh)
return P*mkvc(u)
def getRhs(self, mesh):
if mesh not in self._rhsDict:
RHS = np.array([src.getRhs(mesh) for src in self.srcList]).T
self._rhsDict[mesh] = RHS
return self._rhsDict[mesh]
def getP(self, mesh):
if mesh in self._Ps:
return self._Ps[mesh]
P_src = [sp.vstack([rx.getP(mesh) for rx in src.rxList]) for src in self.srcList]
self._Ps[mesh] = sp.block_diag(P_src)
return self._Ps[mesh]
class ProblemDC(Problem.BaseProblem):
"""
**ProblemDC**
Geophysical DC resistivity problem.
"""
surveyPair = SurveyDC
Solver = Solver
def __init__(self, mesh, **kwargs):
Problem.BaseProblem.__init__(self, mesh)
self.mesh.setCellGradBC('neumann')
Utils.setKwargs(self, **kwargs)
deleteTheseOnModelUpdate = ['_A', '_Msig', '_dMdsig']
@property
def Msig(self):
if getattr(self, '_Msig', None) is None:
sigma = self.curModel.transform
Av = self.mesh.aveF2CC
self._Msig = Utils.sdiag(1/(self.mesh.dim * Av.T * (1/sigma)))
return self._Msig
@property
def dMdsig(self):
if getattr(self, '_dMdsig', None) is None:
sigma = self.curModel.transform
Av = self.mesh.aveF2CC
dMdprop = self.mesh.dim * Utils.sdiag(self.Msig.diagonal()**2) * Av.T * Utils.sdiag(1./sigma**2)
self._dMdsig = lambda Gu: Utils.sdiag(Gu) * dMdprop
return self._dMdsig
@property
def A(self):
"""
Makes the matrix A(m) for the DC resistivity problem.
:param numpy.array m: model
:rtype: scipy.csc_matrix
:return: A(m)
.. math::
c(m,u) = A(m)u - q = G\\text{sdiag}(M(mT(m)))Du - q = 0
Where M() is the mass matrix and mT is the model transform.
"""
if getattr(self, '_A', None) is None:
D = self.mesh.faceDiv
G = self.mesh.cellGrad
self._A = D*self.Msig*G
# Remove the null space from the matrix.
self._A[-1,-1] /= self.mesh.vol[-1]
self._A = self._A.tocsc()
return self._A
def fields(self, m):
self.curModel = m
A = self.A
Ainv = self.Solver(A, **self.solverOpts)
Q = self.survey.getRhs(self.mesh)
Phi = Ainv * Q
return Phi
def Jvec(self, m, v, u=None):
"""
:param numpy.array m: model
:param numpy.array v: vector to multiply
:param numpy.array u: fields
:rtype: numpy.array
:return: Jv
.. math::
c(m,u) = A(m)u - q = G\\text{sdiag}(M(mT(m)))Du - q = 0
\\nabla_u (A(m)u - q) = A(m)
\\nabla_m (A(m)u - q) = G\\text{sdiag}(Du)\\nabla_m(M(mT(m)))
Where M() is the mass matrix and mT is the model transform.
.. math::
J = - P \left( \\nabla_u c(m, u) \\right)^{-1} \\nabla_m c(m, u)
J(v) = - P ( A(m)^{-1} ( G\\text{sdiag}(Du)\\nabla_m(M(mT(m))) v ) )
"""
# Set current model; clear dependent property $\mathbf{A(m)}$
self.curModel = m
sigma = self.curModel.transform # $\sigma = \mathcal{M}(\m)$
if u is None:
# Run forward simulation if $u$ not provided
u = self.fields(self.curModel)
else:
shp = (self.mesh.nC, self.survey.nSrc)
u = u.reshape(shp, order='F')
D = self.mesh.faceDiv
G = self.mesh.cellGrad
# Derivative of model transform, $\deriv{\sigma}{\m}$
dsigdm_x_v = self.curModel.transformDeriv * v
# Take derivative of $C(m,u)$ w.r.t. $m$
dCdm_x_v = np.empty_like(u)
# loop over fields for each source
for i in range(self.survey.nSrc):
# Derivative of inner product, $\left(\mathbf{M}_{1/\sigma}^f\right)^{-1}$
dAdsig = D * self.dMdsig( G * u[:,i] )
dCdm_x_v[:, i] = dAdsig * dsigdm_x_v
# Take derivative of $C(m,u)$ w.r.t. $u$
dCdu = self.A
# Solve for $\deriv{u}{m}$
dCdu_inv = self.Solver(dCdu, **self.solverOpts)
P = self.survey.getP(self.mesh)
J_x_v = - P * mkvc( dCdu_inv * dCdm_x_v )
return J_x_v
def Jtvec(self, m, v, u=None):
self.curModel = m
sigma = self.curModel.transform # $\sigma = \mathcal{M}(\m)$
if u is None:
u = self.fields(self.curModel)
shp = (self.mesh.nC, self.survey.nSrc)
u = u.reshape(shp, order='F')
P = self.survey.getP(self.mesh)
PT_x_v = (P.T*v).reshape(shp, order='F')
D = self.mesh.faceDiv
G = self.mesh.cellGrad
A = self.A
mT_dm = self.mapping.deriv(m)
dCdu = A.T
Ainv = self.Solver(dCdu, **self.solverOpts)
w = Ainv * PT_x_v
Jtv = 0
for i, ui in enumerate(u.T): # loop over each column
Jtv += self.dMdsig( G * ui ).T * ( D.T * w[:,i] )
Jtv = - mT_dm.T * ( Jtv )
return Jtv