Merge branch 'em/dev' into em/ref/tdem

# Conflicts:
#	SimPEG/EM/FDEM/FDEM.py
#	SimPEG/EM/FDEM/SrcFDEM.py
#	SimPEG/EM/FDEM/SurveyFDEM.py
#	SimPEG/Examples/EM_FDEM_1D_Inversion.py
This commit is contained in:
Lindsey Heagy
2016-05-11 09:21:59 -07:00
73 changed files with 5852 additions and 1239 deletions
+1 -1
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@@ -1,4 +1,4 @@
[bumpversion]
current_version = 0.1.9
current_version = 0.1.10
files = setup.py SimPEG/__init__.py docs/conf.py
+1
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@@ -18,6 +18,7 @@ env:
- TEST_DIR="tests/mesh tests/base tests/utils"
- TEST_DIR=tests/em/fdem/inverse/derivs
- TEST_DIR=tests/em/tdem
- TEST_DIR=tests/dcip
- TEST_DIR=tests/flow
- TEST_DIR=tests/mt
- TEST_DIR=tests/examples
+4
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@@ -25,6 +25,10 @@ SimPEG
:target: https://coveralls.io/r/simpeg/simpeg?branch=master
:alt: Coverage status
.. image:: http://img.shields.io/badge/GITTER-JOIN_CHAT-brightgreen.svg?style=flat-square
:alt: gitter chat room at https://gitter.im/simpeg/simpeg
:target: https://gitter.im/simpeg/simpeg
Simulation and Parameter Estimation in Geophysics - A python package for simulation and gradient based parameter estimation in the context of geophysical applications.
The vision is to create a package for finite volume simulation with applications to geophysical imaging and subsurface flow. To enable the understanding of the many different components, this package has the following features:
+292
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@@ -0,0 +1,292 @@
from SimPEG import *
class FieldsDC_CC(Problem.Fields):
knownFields = {'phi_sol':'CC'}
aliasFields = {
'phi' : ['phi_sol','CC','_phi'],
'e' : ['phi_sol','F','_e'],
'j' : ['phi_sol','F','_j']
}
def __init__(self,mesh,survey,**kwargs):
super(FieldsDC_CC, self).__init__(mesh, survey, **kwargs)
def startup(self):
self._cellGrad = self.survey.prob.mesh.cellGrad
self._Mfinv = self.survey.prob.mesh.getFaceInnerProduct(invMat=True)
def _phi(self, phi_sol, srcList):
phi = phi_sol
# for i, src in enumerate(srcList):
# phi_p = src.phi_p(self.survey.prob)
# if phi_p is not None:
# phi[:,i] += phi_p
return phi
def _e(self, phi_sol, srcList):
e = -self._cellGrad*phi_sol
# for i, src in enumerate(srcList):
# e_p = src.e_p(self.survey.prob)
# if e_p is not None:
# e[:,i] += e_p
return e
def _j(self, phi_sol, srcList):
j = -self._Mfinv*self.survey.prob.Msig*self._cellGrad*phi_sol
# for i, src in enumerate(srcList):
# j_p = src.j_p(self.survey.prob)
# if j_p is not None:
# j[:,i] += j_p
return j
class SrcDipole(Survey.BaseSrc):
"""A dipole source, locA and locB are moved to the closest cell-centers"""
current = 1
loc = None
# _rhsDict = None
def __init__(self, rxList, locA, locB, **kwargs):
self.loc = (locA, locB)
super(SrcDipole, self).__init__(rxList, **kwargs)
def eval(self, prob):
# Recompute rhs
# if getattr(self, '_rhsDict', None) is None:
# self._rhsDict = {}
# if mesh not in self._rhsDict:
pts = [self.loc[0], self.loc[1]]
inds = Utils.closestPoints(prob.mesh, pts)
q = np.zeros(prob.mesh.nC)
q[inds] = - self.current * ( np.r_[1., -1.] / prob.mesh.vol[inds] )
# self._rhsDict[mesh] = q
# return self._rhsDict[mesh]
return q
class RxDipole(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(RxDipole, 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.
"""
uncert = None
def __init__(self, srcList, **kwargs):
self.srcList = srcList
Survey.BaseSurvey.__init__(self, **kwargs)
# self._rhsDict = {}
self._Ps = {}
def eval(self, u):
"""
Predicted data.
.. math::
d_\\text{pred} = Pu(m)
"""
P = self.getP(self.prob.mesh)
return P*mkvc(u[self.srcList, 'phi_sol'])
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_CC(Problem.BaseProblem):
"""
**ProblemDC**
Geophysical DC resistivity problem.
"""
surveyPair = SurveyDC
Solver = Solver
fieldsPair = FieldsDC_CC
Ainv = None
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[0,0] /= self.mesh.vol[0]
self._A = self._A.tocsc()
return self._A
def getRHS(self):
# if self.mesh not in self._rhsDict:
RHS = np.array([src.eval(self) for src in self.survey.srcList]).T
# self._rhsDict[mesh] = RHS
# return self._rhsDict[mesh]
return RHS
def fields(self, m):
F = self.fieldsPair(self.mesh, self.survey)
self.curModel = m
A = self.A
self.Ainv = self.Solver(A, **self.solverOpts)
RHS = self.getRHS()
Phi = self.Ainv * RHS
Srcs = self.survey.srcList
F[Srcs, 'phi_sol'] = Phi
return F
def Jvec(self, m, v, f=None):
"""
:param numpy.array m: model
:param numpy.array v: vector to multiply
:param Fields f: 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 f is None:
# Run forward simulation if $u$ not provided
f = self.fields(self.curModel)
u = f[self.survey.srcList, 'phi_sol']
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. $u$
dA_du = self.A
# Solve for $\deriv{u}{m}$
# dCdu_inv = self.Solver(dCdu, **self.solverOpts)
if self.Ainv is None:
self.Ainv = self.Solver(dA_du, **self.solverOpts)
P = self.survey.getP(self.mesh)
Jv = - P * mkvc( self.Ainv * dCdm_x_v )
return Jv
def Jtvec(self, m, v, f=None):
self.curModel = m
sigma = self.curModel.transform # $\sigma = \mathcal{M}(\m)$
if f is None:
# Run forward simulation if $f$ not provided
f = self.fields(self.curModel)
u = f[self.survey.srcList, 'phi_sol']
shp = u.shape
P = self.survey.getP(self.mesh)
PT_x_v = (P.T*v).reshape(shp, order='F')
D = self.mesh.faceDiv
G = self.mesh.cellGrad
dA_du = self.A
mT_dm = self.mapping.deriv(m)
# We probably always need this due to the linesearch .. (?)
self.Ainv = self.Solver(dA_du.T, **self.solverOpts)
# if self.Ainv is None:
# self.Ainv = self.Solver(dCdu, **self.solverOpts)
w = self.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
+182
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@@ -0,0 +1,182 @@
from SimPEG import *
from BaseDC import SurveyDC, FieldsDC_CC
class SurveyIP(SurveyDC):
"""
**SurveyDC**
Geophysical DC resistivity data.
"""
def __init__(self, srcList, **kwargs):
self.srcList = srcList
Survey.BaseSurvey.__init__(self, **kwargs)
self._Ps = {}
def dpred(self, m, f=None):
"""
Predicted data.
.. math::
d_\\text{pred} = Pf(m)
"""
return self.prob.forward(m)
class ProblemIP(Problem.BaseProblem):
"""
**ProblemIP**
Geophysical IP resistivity problem.
"""
surveyPair = SurveyDC
Solver = Solver
sigma = None
Ainv = None
u = None
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
sigma = self.sigma
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
sigma = self.sigma
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 getRHS(self):
# if self.mesh not in self._rhsDict:
RHS = np.array([src.eval(self) for src in self.survey.srcList]).T
# self._rhsDict[mesh] = RHS
# return self._rhsDict[mesh]
return RHS
def fields(self, m):
if self.u is None:
A = self.A
if self.Ainv == None:
self.Ainv = self.Solver(A, **self.solverOpts)
Q = self.getRHS()
self.u = self.Ainv * Q
return self.u
def forward(self, m, u=None):
# Set current model; clear dependent property $\mathbf{A(m)}$
self.curModel = m
# sigma = self.curModel.transform # $\sigma = \mathcal{M}(\m)$
sigma = self.sigma
if self.u is None:
# Run forward simulation if $u$ not provided
u = self.fields(sigma)
shp = (self.mesh.nC, self.survey.nSrc)
u = self.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
dsigdm_x_v = Utils.sdiag(sigma) * self.curModel.transformDeriv * m
# 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. $u$
if self.Ainv == None:
self.Ainv = self.Solver(A, **self.solverOpts)
# 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( self.Ainv * dCdm_x_v )
return -J_x_v
def Jvec(self, m, v, f=None):
return self.forward(v)
def Jtvec(self, m, v, f=None):
self.curModel = m
# sigma = self.curModel.transform # $\sigma = \mathcal{M}(\m)$
sigma = self.sigma
if self.u is None:
u = self.fields(sigma)
else:
u = self.u
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 = Utils.sdiag(sigma)*self.mapping.deriv(m)
# mT_dm = self.mapping.deriv(m)
# dCdu = A.T
# Ainv = self.Solver(dCdu, **self.solverOpts)
# if self.Ainv == None:
self.Ainv = self.Solver(A.T, **self.solverOpts)
w = self.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
File diff suppressed because it is too large Load Diff
+38
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@@ -0,0 +1,38 @@
import numpy as np
def WennerSrcList(nElecs, aSpacing, in2D=False, plotIt=False):
import SimPEG.DCIP as DC
elocs = np.arange(0,aSpacing*nElecs,aSpacing)
elocs -= (nElecs*aSpacing - aSpacing)/2
space = 1
WENNER = np.zeros((0,),dtype=int)
for ii in range(nElecs):
for jj in range(nElecs):
test = np.r_[jj,jj+space,jj+space*2,jj+space*3]
if np.any(test >= nElecs):
break
WENNER = np.r_[WENNER, test]
space += 1
WENNER = WENNER.reshape((-1,4))
if plotIt:
for i, s in enumerate('rbkg'):
plt.plot(elocs[WENNER[:,i]],s+'.')
plt.show()
# Create sources and receivers
i = 0
if in2D:
getLoc = lambda ii, abmn: np.r_[elocs[WENNER[ii,abmn]],0]
else:
getLoc = lambda ii, abmn: np.r_[elocs[WENNER[ii,abmn]],0, 0]
srcList = []
for i in range(WENNER.shape[0]):
rx = DC.RxDipole(getLoc(i,1),getLoc(i,2))
src = DC.SrcDipole([rx], getLoc(i,0),getLoc(i,3))
srcList += [src]
return srcList
+4
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@@ -0,0 +1,4 @@
from BaseDC import *
from BaseIP import *
from DCIPUtils import *
import Utils
+22 -26
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@@ -22,11 +22,11 @@ class BaseDataMisfit(object):
Utils.setKwargs(self,**kwargs)
@Utils.timeIt
def eval(self, m, u=None):
"""eval(m, u=None)
def eval(self, m, f=None):
"""eval(m, f=None)
:param numpy.array m: geophysical model
:param numpy.array u: fields
:param Fields f: fields
:rtype: float
:return: data misfit
@@ -34,11 +34,11 @@ class BaseDataMisfit(object):
raise NotImplementedError('This method should be overwritten.')
@Utils.timeIt
def evalDeriv(self, m, u=None):
"""evalDeriv(m, u=None)
def evalDeriv(self, m, f=None):
"""evalDeriv(m, f=None)
:param numpy.array m: geophysical model
:param numpy.array u: fields
:param Fields f: fields
:rtype: numpy.array
:return: data misfit derivative
@@ -47,12 +47,12 @@ class BaseDataMisfit(object):
@Utils.timeIt
def eval2Deriv(self, m, v, u=None):
"""eval2Deriv(m, v, u=None)
def eval2Deriv(self, m, v, f=None):
"""eval2Deriv(m, v, f=None)
:param numpy.array m: geophysical model
:param numpy.array v: vector to multiply
:param numpy.array u: fields
:param Fields f: fields
:rtype: numpy.array
:return: data misfit derivative
@@ -89,7 +89,7 @@ class l2_DataMisfit(BaseDataMisfit):
"""
if getattr(self, '_Wd', None) is None:
survey = self.survey
if getattr(survey,'std', None) is None:
@@ -108,24 +108,20 @@ class l2_DataMisfit(BaseDataMisfit):
self._Wd = value
@Utils.timeIt
def eval(self, m, u=None):
"eval(m, u=None)"
prob = self.prob
survey = self.survey
R = self.Wd * survey.residual(m, u=u)
def eval(self, m, f=None):
"eval(m, f=None)"
if f is None: f = self.prob.fields(m)
R = self.Wd * self.survey.residual(m, f)
return 0.5*np.vdot(R, R)
@Utils.timeIt
def evalDeriv(self, m, u=None):
"evalDeriv(m, u=None)"
prob = self.prob
survey = self.survey
if u is None: u = prob.fields(m)
return prob.Jtvec(m, self.Wd * (self.Wd * survey.residual(m, u=u)), u=u)
def evalDeriv(self, m, f=None):
"evalDeriv(m, f=None)"
if f is None: f = self.prob.fields(m)
return self.prob.Jtvec(m, self.Wd * (self.Wd * self.survey.residual(m, f=f)), f=f)
@Utils.timeIt
def eval2Deriv(self, m, v, u=None):
"eval2Deriv(m, v, u=None)"
prob = self.prob
if u is None: u = prob.fields(m)
return prob.Jtvec_approx(m, self.Wd * (self.Wd * prob.Jvec_approx(m, v, u=u)), u=u)
def eval2Deriv(self, m, v, f=None):
"eval2Deriv(m, v, f=None)"
if f is None: f = self.prob.fields(m)
return self.prob.Jtvec_approx(m, self.Wd * (self.Wd * self.prob.Jvec_approx(m, v, f=f)), f=f)
+126 -38
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@@ -123,10 +123,10 @@ class BetaEstimate_ByEig(InversionDirective):
if self.debug: print 'Calculating the beta0 parameter.'
m = self.invProb.curModel
u = self.invProb.getFields(m, store=True, deleteWarmstart=False)
f = self.invProb.getFields(m, store=True, deleteWarmstart=False)
x0 = np.random.rand(*m.shape)
t = x0.dot(self.dmisfit.eval2Deriv(m,x0,u=u))
t = x0.dot(self.dmisfit.eval2Deriv(m,x0,f=f))
b = x0.dot(self.reg.eval2Deriv(m, v=x0))
self.beta0 = self.beta0_ratio*(t/b)
@@ -216,13 +216,13 @@ class SaveOutputDictEveryIteration(_SaveEveryIteration):
# Save the data.
ms = self.reg.Ws * ( self.reg.mapping * (self.invProb.curModel - self.reg.mref) )
phi_ms = 0.5*ms.dot(ms)
if self.reg.smoothModel == True:
if self.reg.mrefInSmooth == True:
mref = self.reg.mref
else:
mref = 0
mx = self.reg.Wx * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_mx = 0.5 * mx.dot(mx)
if self.prob.mesh.dim==2:
if self.prob.mesh.dim >= 2:
my = self.reg.Wy * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_my = 0.5 * my.dot(my)
else:
@@ -237,40 +237,6 @@ class SaveOutputDictEveryIteration(_SaveEveryIteration):
# Save the file as a npz
np.savez('{:03d}-{:s}'.format(self.opt.iter,self.fileName), iter=self.opt.iter, beta=self.invProb.beta, phi_d=self.invProb.phi_d, phi_m=self.invProb.phi_m, phi_ms=phi_ms, phi_mx=phi_mx, phi_my=phi_my, phi_mz=phi_mz,f=self.opt.f, m=self.invProb.curModel,dpred=self.invProb.dpred)
class SaveOutputDictEveryIteration(_SaveEveryIteration):
"""SaveOutputDictEveryIteration
A directive that saves some relevant information from the inversion run to a numpy .npz dictionary file (see numpy.savez function for further info).
"""
def initialize(self):
print "SimPEG.SaveOutputDictEveryIteration will save your inversion progress as dictionary: '%s-###.npz'"%self.fileName
def endIter(self):
# Save the data.
ms = self.reg.Ws * ( self.reg.mapping * (self.invProb.curModel - self.reg.mref) )
phi_ms = 0.5*ms.dot(ms)
if self.reg.smoothModel == True:
mref = self.reg.mref
else:
mref = 0
mx = self.reg.Wx * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_mx = 0.5 * mx.dot(mx)
if self.prob.mesh.dim==2:
my = self.reg.Wy * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_my = 0.5 * my.dot(my)
else:
phi_my = 'NaN'
if self.prob.mesh.dim==3 and 'CYL' not in self.prob.mesh._meshType:
mz = self.reg.Wz * ( self.reg.mapping * (self.invProb.curModel - mref) )
phi_mz = 0.5 * mz.dot(mz)
else:
phi_mz = 'NaN'
# Save the file as a npz
np.savez('{:s}-{:03d}'.format(self.fileName,self.opt.iter), iter=self.opt.iter, beta=self.invProb.beta, phi_d=self.invProb.phi_d, phi_m=self.invProb.phi_m, phi_ms=phi_ms, phi_mx=phi_mx, phi_my=phi_my, phi_mz=phi_mz,f=self.opt.f, m=self.invProb.curModel,dpred=self.invProb.dpred)
# class UpdateReferenceModel(Parameter):
@@ -283,3 +249,125 @@ class SaveOutputDictEveryIteration(_SaveEveryIteration):
# mref = self.mref0
# self.m_prev = self.invProb.m_current
# return mref
class Update_IRLS(InversionDirective):
eps_min = None
factor = None
gamma = None
phi_m_last = None
phi_d_last = None
def initialize(self):
# Scale the regularization for changes in norm
if getattr(self, 'phi_m_last', None) is not None:
self.reg.curModel = self.invProb.curModel
self.reg.gamma = 1.
phim_new = self.reg.eval(self.invProb.curModel)
self.gamma = self.phi_m_last / phim_new
self.reg.curModel = self.invProb.curModel
self.reg.gamma = self.gamma
if getattr(self, 'phi_d_last', None) is None:
self.phi_d_last = self.invProb.phi_d
def endIter(self):
# Cool the threshold parameter if required
if getattr(self, 'factor', None) is not None:
eps = self.reg.eps / self.factor
if getattr(self, 'eps_min', None) is not None:
self.reg.eps = np.max([self.eps_min,eps])
else:
self.reg.eps = eps
# Get phi_m at the end of current iteration
self.phi_m_last = self.invProb.phi_m_last
# Update the model used for the IRLS weights
self.reg.curModel = self.invProb.curModel
# Temporarely set gamma to 1. to get raw phi_m
self.reg.gamma = 1.
# Compute new model objective function value
phim_new = self.reg.eval(self.invProb.curModel)
# Update gamma to scale the regularization between IRLS iterations
self.reg.gamma = self.phi_m_last / phim_new
# Set the weighting matrix to None so that it is recomputed next time
# it is called in the inversion
self.reg._W = None
class Update_lin_PreCond(InversionDirective):
"""
Create a Jacobi preconditioner for the linear problem
"""
onlyOnStart=False
def initialize(self):
if getattr(self.opt, 'approxHinv', None) is None:
# Update the pre-conditioner
diagA = np.sum(self.prob.G**2.,axis=0) + self.invProb.beta*(self.reg.W.T*self.reg.W).diagonal() #* (self.reg.mapping * np.ones(self.reg.curModel.size))**2.
PC = Utils.sdiag((self.prob.mapping.deriv(None).T *diagA)**-1.)
self.opt.approxHinv = PC
def endIter(self):
# Cool the threshold parameter
if self.onlyOnStart==True:
return
if getattr(self.opt, 'approxHinv', None) is not None:
# Update the pre-conditioner
diagA = np.sum(self.prob.G**2.,axis=0) + self.invProb.beta*(self.reg.W.T*self.reg.W).diagonal() #* (self.reg.mapping * np.ones(self.reg.curModel.size))**2.
PC = Utils.sdiag((self.prob.mapping.deriv(None).T *diagA)**-1.)
self.opt.approxHinv = PC
class Update_Wj(InversionDirective):
"""
Create approx-sensitivity base weighting using the probing method
"""
k = None # Number of probing cycles
itr = None # Iteration number to update Wj, or always update if None
def endIter(self):
if self.itr is None or self.itr == self.opt.iter:
m = self.invProb.curModel
if self.k is None:
self.k = int(self.survey.nD/10)
def JtJv(v):
Jv = self.prob.Jvec(m, v)
return self.prob.Jtvec(m,Jv)
JtJdiag = Utils.diagEst(JtJv,len(m),k=self.k)
JtJdiag = JtJdiag / max(JtJdiag)
self.reg.wght = JtJdiag
class Scale_Beta(InversionDirective):
"""
Instead of a linear cooling schedule, beta is allowed to change based
on the ratio between the target misfit and the current data misfit. The
update is done only if the misfit is outside some threshold bounds.
"""
tol = 0.05
def endIter(self):
# Check if misfit is within the tolerance, otherwise adjust beta
val = self.invProb.phi_d / (self.survey.nD*0.5)
if np.abs(1.-val) > self.tol:
self.invProb.beta = self.invProb.beta * self.survey.nD*0.5 / self.invProb.phi_d
+55 -14
View File
@@ -2,14 +2,14 @@ from SimPEG import Survey, Problem, Utils, Models, Maps, PropMaps, np, sp, Solve
from scipy.constants import mu_0
class EMPropMap(Maps.PropMap):
"""
"""
Property Map for EM Problems. The electrical conductivity (\\(\\sigma\\)) is the default inversion property, and the default value of the magnetic permeability is that of free space (\\(\\mu = 4\\pi\\times 10^{-7} \\) H/m)
"""
sigma = Maps.Property("Electrical Conductivity", defaultInvProp = True, propertyLink=('rho',Maps.ReciprocalMap))
mu = Maps.Property("Inverse Magnetic Permeability", defaultVal = mu_0, propertyLink=('mui',Maps.ReciprocalMap))
rho = Maps.Property("Electrical Resistivity", propertyLink=('sigma', Maps.ReciprocalMap))
rho = Maps.Property("Electrical Resistivity", propertyLink=('sigma', Maps.ReciprocalMap))
mui = Maps.Property("Inverse Magnetic Permeability", defaultVal = 1./mu_0, propertyLink=('mu', Maps.ReciprocalMap))
@@ -21,7 +21,7 @@ class BaseEMProblem(Problem.BaseProblem):
surveyPair = Survey.BaseSurvey
dataPair = Survey.Data
PropMap = EMPropMap
Solver = SimpegSolver
@@ -51,7 +51,7 @@ class BaseEMProblem(Problem.BaseProblem):
if self.mapping.muMap is not None or self.mapping.muiMap is not None:
toDelete += ['_MeMu', '_MeMuI','_MfMui','_MfMuiI']
return toDelete
@property
def Me(self):
"""
@@ -61,6 +61,15 @@ class BaseEMProblem(Problem.BaseProblem):
self._Me = self.mesh.getEdgeInnerProduct()
return self._Me
@property
def MeI(self):
"""
Edge inner product matrix
"""
if getattr(self, '_MeI', None) is None:
self._MeI = self.mesh.getEdgeInnerProduct(invMat=True)
return self._MeI
@property
def Mf(self):
"""
@@ -70,8 +79,17 @@ class BaseEMProblem(Problem.BaseProblem):
self._Mf = self.mesh.getFaceInnerProduct()
return self._Mf
@property
def MfI(self):
"""
Face inner product matrix
"""
if getattr(self, '_MfI', None) is None:
self._MfI = self.mesh.getFaceInnerProduct(invMat=True)
return self._MfI
# ----- Magnetic Permeability ----- #
# ----- Magnetic Permeability ----- #
@property
def MfMui(self):
"""
@@ -109,7 +127,7 @@ class BaseEMProblem(Problem.BaseProblem):
return self._MeMuI
# ----- Electrical Conductivity ----- #
# ----- Electrical Conductivity ----- #
#TODO: hardcoded to sigma as the model
@property
def MeSigma(self):
@@ -120,18 +138,18 @@ class BaseEMProblem(Problem.BaseProblem):
self._MeSigma = self.mesh.getEdgeInnerProduct(self.curModel.sigma)
return self._MeSigma
# TODO: This should take a vector
# TODO: This should take a vector
def MeSigmaDeriv(self, u):
"""
Derivative of MeSigma with respect to the model
"""
"""
return self.mesh.getEdgeInnerProductDeriv(self.curModel.sigma)(u) * self.curModel.sigmaDeriv
@property
def MeSigmaI(self):
"""
Inverse of the edge inner product matrix for \\(\\sigma\\).
Inverse of the edge inner product matrix for \\(\\sigma\\).
"""
if getattr(self, '_MeSigmaI', None) is None:
self._MeSigmaI = self.mesh.getEdgeInnerProduct(self.curModel.sigma, invMat=True)
@@ -140,8 +158,8 @@ class BaseEMProblem(Problem.BaseProblem):
# TODO: This should take a vector
def MeSigmaIDeriv(self, u):
"""
Derivative of :code:`MeSigma` with respect to the model
"""
Derivative of :code:`MeSigma` with respect to the model
"""
# TODO: only works for diagonal tensors. getEdgeInnerProductDeriv, invMat=True should be implemented in SimPEG
dMeSigmaI_dI = -self.MeSigmaI**2
@@ -163,7 +181,7 @@ class BaseEMProblem(Problem.BaseProblem):
# TODO: This should take a vector
def MfRhoDeriv(self,u):
"""
Derivative of :code:`MfRho` with respect to the model.
Derivative of :code:`MfRho` with respect to the model.
"""
return self.mesh.getFaceInnerProductDeriv(self.curModel.rho)(u) * (-Utils.sdiag(self.curModel.rho**2) * self.curModel.sigmaDeriv)
# self.curModel.rhoDeriv
@@ -181,6 +199,29 @@ class BaseEMProblem(Problem.BaseProblem):
# TODO: This should take a vector
def MfRhoIDeriv(self,u):
"""
Derivative of :code:`MfRhoI` with respect to the model.
Derivative of :code:`MfRhoI` with respect to the model.
"""
return self.mesh.getFaceInnerProductDeriv(self.curModel.rho, invMat=True)(u) * self.curModel.rhoDeriv
class BaseEMSurvey(Survey.BaseSurvey):
def __init__(self, srcList, **kwargs):
# Sort these by frequency
self.srcList = srcList
Survey.BaseSurvey.__init__(self, **kwargs)
def eval(self, u):
"""
Project fields to receiver locations
:param Fields u: fields object
:rtype: numpy.ndarray
:return: data
"""
data = Survey.Data(self)
for src in self.srcList:
for rx in src.rxList:
data[src, rx] = rx.eval(src, self.mesh, u)
return data
def evalDeriv(self, u):
raise Exception('Use Receivers to project fields deriv.')
+78 -83
View File
@@ -1,7 +1,7 @@
from SimPEG import Problem, Utils, np, sp, Solver as SimpegSolver
from scipy.constants import mu_0
from SurveyFDEM import Survey as SurveyFDEM
from FieldsFDEM import Fields, Fields_e, Fields_b, Fields_h, Fields_j
from FieldsFDEM import Fields, Fields3D_e, Fields3D_b, Fields3D_h, Fields3D_j
from SimPEG.EM.Base import BaseEMProblem
from SimPEG.EM.Utils import omega
@@ -17,8 +17,8 @@ class BaseFDEMProblem(BaseEMProblem):
\mathbf{C} \mathbf{e} + i \omega \mathbf{b} = \mathbf{s_m} \\\\
{\mathbf{C}^{\\top} \mathbf{M_{\mu^{-1}}^f} \mathbf{b} - \mathbf{M_{\sigma}^e} \mathbf{e} = \mathbf{s_e}}
if using the E-B formulation (:code:`Problem_e`
or :code:`Problem_b`). Note that in this case, :math:`\mathbf{s_e}` is an integrated quantity.
if using the E-B formulation (:code:`Problem3D_e`
or :code:`Problem3D_b`). Note that in this case, :math:`\mathbf{s_e}` is an integrated quantity.
If we write Maxwell's equations in terms of
\\\(\\\mathbf{h}\\\) and current density \\\(\\\mathbf{j}\\\)
@@ -28,7 +28,7 @@ class BaseFDEMProblem(BaseEMProblem):
\mathbf{C}^{\\top} \mathbf{M_{\\rho}^f} \mathbf{j} + i \omega \mathbf{M_{\mu}^e} \mathbf{h} = \mathbf{s_m} \\\\
\mathbf{C} \mathbf{h} - \mathbf{j} = \mathbf{s_e}
if using the H-J formulation (:code:`Problem_j` or :code:`Problem_h`). Note that here, :math:`\mathbf{s_m}` is an integrated quantity.
if using the H-J formulation (:code:`Problem3D_j` or :code:`Problem3D_h`). Note that here, :math:`\mathbf{s_m}` is an integrated quantity.
The problem performs the elimination so that we are solving the system for \\\(\\\mathbf{e},\\\mathbf{b},\\\mathbf{j} \\\) or \\\(\\\mathbf{h}\\\)
"""
@@ -36,30 +36,29 @@ class BaseFDEMProblem(BaseEMProblem):
surveyPair = SurveyFDEM
fieldsPair = Fields
def fields(self, m=None):
def fields(self, m):
"""
Solve the forward problem for the fields.
:param numpy.array m: inversion model (nP,)
:rtype numpy.array:
:return F: forward solution
:return f: forward solution
"""
self.curModel = m
F = self.fieldsPair(self.mesh, self.survey)
f = self.fieldsPair(self.mesh, self.survey)
for freq in self.survey.freqs:
A = self.getA(freq)
rhs = self.getRHS(freq)
Ainv = self.Solver(A, **self.solverOpts)
sol = Ainv * rhs
u = Ainv * rhs
Srcs = self.survey.getSrcByFreq(freq)
ftype = self._fieldType + 'Solution'
F[Srcs, ftype] = sol
f[Srcs, self._solutionType] = u
Ainv.clean()
return F
return f
def Jvec(self, m, v, u=None):
def Jvec(self, m, v, f=None):
"""
Sensitivity times a vector.
@@ -70,33 +69,31 @@ class BaseFDEMProblem(BaseEMProblem):
:return: Jv (ndata,)
"""
if u is None:
u = self.fields(m)
if f is None:
f = self.fields(m)
self.curModel = m
Jv = self.dataPair(self.survey)
for freq in self.survey.freqs:
A = self.getA(freq) #
Ainv = self.Solver(A, **self.solverOpts)
A = self.getA(freq)
Ainv = self.Solver(A, **self.solverOpts) # create the concept of Ainv (actually a solve)
for src in self.survey.getSrcByFreq(freq):
ftype = self._fieldType + 'Solution'
u_src = u[src, ftype]
u_src = f[src, self._solutionType]
dA_dm_v = self.getADeriv(freq, u_src, v)
dRHS_dm_v = self.getRHSDeriv(freq, src, v)
du_dm_v = Ainv * ( - dA_dm_v + dRHS_dm_v )
for rx in src.rxList:
df_dmFun = getattr(u, '_%sDeriv'%rx.projField, None)
df_dmFun = getattr(f, '_%sDeriv'%rx.projField, None)
df_dm_v = df_dmFun(src, du_dm_v, v, adjoint=False)
df_dm_v = np.array(df_dm_v, dtype=complex)
Jv[src, rx] = rx.evalDeriv(src, self.mesh, u, df_dm_v)
Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v)
Ainv.clean()
return Utils.mkvc(Jv)
def Jtvec(self, m, v, u=None):
def Jtvec(self, m, v, f=None):
"""
Sensitivity transpose times a vector
@@ -107,8 +104,8 @@ class BaseFDEMProblem(BaseEMProblem):
:return: Jv (ndata,)
"""
if u is None:
u = self.fields(m)
if f is None:
f = self.fields(m)
self.curModel = m
@@ -123,13 +120,12 @@ class BaseFDEMProblem(BaseEMProblem):
ATinv = self.Solver(AT, **self.solverOpts)
for src in self.survey.getSrcByFreq(freq):
ftype = self._fieldType + 'Solution'
u_src = u[src, ftype]
u_src = f[src, self._solutionType]
for rx in src.rxList:
PTv = rx.evalDeriv(src, self.mesh, u, v[src, rx], adjoint=True) # wrt u, need possibility wrt m
PTv = rx.evalDeriv(src, self.mesh, f, v[src, rx], adjoint=True) # wrt f, need possibility wrt m
df_duTFun = getattr(u, '_%sDeriv'%rx.projField, None)
df_duTFun = getattr(f, '_%sDeriv'%rx.projField, None)
df_duT, df_dmT = df_duTFun(src, None, PTv, adjoint=True)
ATinvdf_duT = ATinv * df_duT
@@ -138,14 +134,13 @@ class BaseFDEMProblem(BaseEMProblem):
dRHS_dmT = self.getRHSDeriv(freq, src, ATinvdf_duT, adjoint=True)
du_dmT = -dA_dmT + dRHS_dmT
df_dmT += du_dmT
df_dmT = df_dmT + du_dmT
# TODO: this should be taken care of by the reciever?
real_or_imag = rx.projComp
if real_or_imag is 'real':
Jtv += np.array(df_dmT,dtype=complex).real
elif real_or_imag is 'imag':
Jtv += - np.array(df_dmT,dtype=complex).real
if rx.real_or_imag is 'real':
Jtv += np.array(df_dmT, dtype=complex).real
elif rx.real_or_imag is 'imag':
Jtv += - np.array(df_dmT, dtype=complex).real
else:
raise Exception('Must be real or imag')
@@ -159,29 +154,29 @@ class BaseFDEMProblem(BaseEMProblem):
:param float freq: Frequency
:rtype: (numpy.ndarray, numpy.ndarray)
:return: S_m, S_e (nE or nF, nSrc)
:return: s_m, s_e (nE or nF, nSrc)
"""
Srcs = self.survey.getSrcByFreq(freq)
if self._eqLocs is 'FE':
S_m = np.zeros((self.mesh.nF,len(Srcs)), dtype=complex)
S_e = np.zeros((self.mesh.nE,len(Srcs)), dtype=complex)
elif self._eqLocs is 'EF':
S_m = np.zeros((self.mesh.nE,len(Srcs)), dtype=complex)
S_e = np.zeros((self.mesh.nF,len(Srcs)), dtype=complex)
if self._formulation is 'EB':
s_m = np.zeros((self.mesh.nF,len(Srcs)), dtype=complex)
s_e = np.zeros((self.mesh.nE,len(Srcs)), dtype=complex)
elif self._formulation is 'HJ':
s_m = np.zeros((self.mesh.nE,len(Srcs)), dtype=complex)
s_e = np.zeros((self.mesh.nF,len(Srcs)), dtype=complex)
for i, src in enumerate(Srcs):
smi, sei = src.eval(self)
S_m[:,i] = S_m[:,i] + smi
S_e[:,i] = S_e[:,i] + sei
s_m[:,i] = s_m[:,i] + smi
s_e[:,i] = s_e[:,i] + sei
return S_m, S_e
return s_m, s_e
##########################################################################################
################################ E-B Formulation #########################################
##########################################################################################
class Problem_e(BaseFDEMProblem):
class Problem3D_e(BaseFDEMProblem):
"""
By eliminating the magnetic flux density using
@@ -201,9 +196,9 @@ class Problem_e(BaseFDEMProblem):
:param SimPEG.Mesh mesh: mesh
"""
_fieldType = 'e'
_eqLocs = 'FE'
fieldsPair = Fields_e
_solutionType = 'eSolution'
_formulation = 'EB'
fieldsPair = Fields3D_e
def __init__(self, mesh, **kwargs):
BaseFDEMProblem.__init__(self, mesh, **kwargs)
@@ -262,11 +257,11 @@ class Problem_e(BaseFDEMProblem):
:return: RHS (nE, nSrc)
"""
S_m, S_e = self.getSourceTerm(freq)
s_m, s_e = self.getSourceTerm(freq)
C = self.mesh.edgeCurl
MfMui = self.MfMui
return C.T * (MfMui * S_m) -1j * omega(freq) * S_e
return C.T * (MfMui * s_m) -1j * omega(freq) * s_e
def getRHSDeriv(self, freq, src, v, adjoint=False):
"""
@@ -282,17 +277,17 @@ class Problem_e(BaseFDEMProblem):
C = self.mesh.edgeCurl
MfMui = self.MfMui
S_mDeriv, S_eDeriv = src.evalDeriv(self, adjoint=adjoint)
s_mDeriv, s_eDeriv = src.evalDeriv(self, adjoint=adjoint)
if adjoint:
dRHS = MfMui * (C * v)
return S_mDeriv(dRHS) - 1j * omega(freq) * S_eDeriv(v)
return s_mDeriv(dRHS) - 1j * omega(freq) * s_eDeriv(v)
else:
return C.T * (MfMui * S_mDeriv(v)) -1j * omega(freq) * S_eDeriv(v)
return C.T * (MfMui * s_mDeriv(v)) -1j * omega(freq) * s_eDeriv(v)
class Problem_b(BaseFDEMProblem):
class Problem3D_b(BaseFDEMProblem):
"""
We eliminate :math:`\mathbf{e}` using
@@ -312,9 +307,9 @@ class Problem_b(BaseFDEMProblem):
:param SimPEG.Mesh mesh: mesh
"""
_fieldType = 'b'
_eqLocs = 'FE'
fieldsPair = Fields_b
_solutionType = 'bSolution'
_formulation = 'EB'
fieldsPair = Fields3D_b
def __init__(self, mesh, **kwargs):
BaseFDEMProblem.__init__(self, mesh, **kwargs)
@@ -387,11 +382,11 @@ class Problem_b(BaseFDEMProblem):
:return: RHS (nE, nSrc)
"""
S_m, S_e = self.getSourceTerm(freq)
s_m, s_e = self.getSourceTerm(freq)
C = self.mesh.edgeCurl
MeSigmaI = self.MeSigmaI
RHS = S_m + C * ( MeSigmaI * S_e )
RHS = s_m + C * ( MeSigmaI * s_e )
if self._makeASymmetric is True:
MfMui = self.MfMui
@@ -412,21 +407,21 @@ class Problem_b(BaseFDEMProblem):
"""
C = self.mesh.edgeCurl
S_m, S_e = src.eval(self)
s_m, s_e = src.eval(self)
MfMui = self.MfMui
if self._makeASymmetric and adjoint:
v = self.MfMui * v
MeSigmaIDeriv = self.MeSigmaIDeriv(S_e)
S_mDeriv, S_eDeriv = src.evalDeriv(self, adjoint=adjoint)
MeSigmaIDeriv = self.MeSigmaIDeriv(s_e)
s_mDeriv, s_eDeriv = src.evalDeriv(self, adjoint=adjoint)
if not adjoint:
RHSderiv = C * (MeSigmaIDeriv * v)
SrcDeriv = S_mDeriv(v) + C * (self.MeSigmaI * S_eDeriv(v))
SrcDeriv = s_mDeriv(v) + C * (self.MeSigmaI * s_eDeriv(v))
elif adjoint:
RHSderiv = MeSigmaIDeriv.T * (C.T * v)
SrcDeriv = S_mDeriv(v) + self.MeSigmaI.T * (C.T * S_eDeriv(v))
SrcDeriv = s_mDeriv(v) + self.MeSigmaI.T * (C.T * s_eDeriv(v))
if self._makeASymmetric is True and not adjoint:
return MfMui.T * (SrcDeriv + RHSderiv)
@@ -440,7 +435,7 @@ class Problem_b(BaseFDEMProblem):
##########################################################################################
class Problem_j(BaseFDEMProblem):
class Problem3D_j(BaseFDEMProblem):
"""
We eliminate \\\(\\\mathbf{h}\\\) using
@@ -460,9 +455,9 @@ class Problem_j(BaseFDEMProblem):
:param SimPEG.Mesh mesh: mesh
"""
_fieldType = 'j'
_eqLocs = 'EF'
fieldsPair = Fields_j
_solutionType = 'jSolution'
_formulation = 'HJ'
fieldsPair = Fields3D_j
def __init__(self, mesh, **kwargs):
BaseFDEMProblem.__init__(self, mesh, **kwargs)
@@ -537,11 +532,11 @@ class Problem_j(BaseFDEMProblem):
:return: RHS
"""
S_m, S_e = self.getSourceTerm(freq)
s_m, s_e = self.getSourceTerm(freq)
C = self.mesh.edgeCurl
MeMuI = self.MeMuI
RHS = C * (MeMuI * S_m) - 1j * omega(freq) * S_e
RHS = C * (MeMuI * s_m) - 1j * omega(freq) * s_e
if self._makeASymmetric is True:
MfRho = self.MfRho
return MfRho.T*RHS
@@ -562,16 +557,16 @@ class Problem_j(BaseFDEMProblem):
C = self.mesh.edgeCurl
MeMuI = self.MeMuI
S_mDeriv, S_eDeriv = src.evalDeriv(self, adjoint=adjoint)
s_mDeriv, s_eDeriv = src.evalDeriv(self, adjoint=adjoint)
if adjoint:
if self._makeASymmetric:
MfRho = self.MfRho
v = MfRho*v
return S_mDeriv(MeMuI.T * (C.T * v)) - 1j * omega(freq) * S_eDeriv(v)
return s_mDeriv(MeMuI.T * (C.T * v)) - 1j * omega(freq) * s_eDeriv(v)
else:
RHSDeriv = C * (MeMuI * S_mDeriv(v)) - 1j * omega(freq) * S_eDeriv(v)
RHSDeriv = C * (MeMuI * s_mDeriv(v)) - 1j * omega(freq) * s_eDeriv(v)
if self._makeASymmetric:
MfRho = self.MfRho
@@ -581,7 +576,7 @@ class Problem_j(BaseFDEMProblem):
class Problem_h(BaseFDEMProblem):
class Problem3D_h(BaseFDEMProblem):
"""
We eliminate \\\(\\\mathbf{j}\\\) using
@@ -598,9 +593,9 @@ class Problem_h(BaseFDEMProblem):
:param SimPEG.Mesh mesh: mesh
"""
_fieldType = 'h'
_eqLocs = 'EF'
fieldsPair = Fields_h
_solutionType = 'hSolution'
_formulation = 'HJ'
fieldsPair = Fields3D_h
def __init__(self, mesh, **kwargs):
BaseFDEMProblem.__init__(self, mesh, **kwargs)
@@ -659,11 +654,11 @@ class Problem_h(BaseFDEMProblem):
:return: RHS (nE, nSrc)
"""
S_m, S_e = self.getSourceTerm(freq)
s_m, s_e = self.getSourceTerm(freq)
C = self.mesh.edgeCurl
MfRho = self.MfRho
return S_m + C.T * ( MfRho * S_e )
return s_m + C.T * ( MfRho * s_e )
def getRHSDeriv(self, freq, src, v, adjoint=False):
"""
@@ -677,17 +672,17 @@ class Problem_h(BaseFDEMProblem):
:return: product of rhs deriv with a vector
"""
_, S_e = src.eval(self)
_, s_e = src.eval(self)
C = self.mesh.edgeCurl
MfRho = self.MfRho
MfRhoDeriv = self.MfRhoDeriv(S_e)
MfRhoDeriv = self.MfRhoDeriv(s_e)
if not adjoint:
RHSDeriv = C.T * (MfRhoDeriv * v)
elif adjoint:
RHSDeriv = MfRhoDeriv.T * (C * v)
S_mDeriv, S_eDeriv = src.evalDeriv(self, adjoint=adjoint)
s_mDeriv, s_eDeriv = src.evalDeriv(self, adjoint=adjoint)
return RHSDeriv + S_mDeriv(v) + C.T * (MfRho * S_eDeriv(v))
return RHSDeriv + s_mDeriv(v) + C.T * (MfRho * s_eDeriv(v))
File diff suppressed because it is too large Load Diff
+126
View File
@@ -0,0 +1,126 @@
import SimPEG
from SimPEG import sp
class BaseRx(SimPEG.Survey.BaseRx):
"""
Frequency domain receiver base class
:param numpy.ndarray locs: receiver locations (ie. :code:`np.r_[x,y,z]`)
:param string orientation: receiver orientation 'x', 'y' or 'z'
:param string real_or_imag: real or imaginary component 'real' or 'imag'
"""
def __init__(self, locs, orientation=None, real_or_imag=None):
assert(orientation in ['x','y','z']), "Orientation %s not known. Orientation must be in 'x', 'y', 'z'. Arbitrary orientations have not yet been implemented."%orientation
assert(real_or_imag in ['real', 'imag']), "'real_or_imag' must be 'real' or 'imag', not %s"%real_or_imag
self.projComp = orientation
self.real_or_imag = real_or_imag
SimPEG.Survey.BaseRx.__init__(self, locs, rxType=None) #TODO: remove rxType from baseRx
def projGLoc(self, u):
"""Grid Location projection (e.g. Ex Fy ...)"""
return u._GLoc(self.projField) + self.projComp
def eval(self, src, mesh, f):
"""
Project fields to recievers to get data.
:param Source src: FDEM source
:param Mesh mesh: mesh used
:param Fields f: fields object
:rtype: numpy.ndarray
:return: fields projected to recievers
"""
P = self.getP(mesh, self.projGLoc(f))
f_part_complex = f[src, self.projField]
f_part = getattr(f_part_complex, self.real_or_imag) # get the real or imag component
return P*f_part
def evalDeriv(self, src, mesh, f, v, adjoint=False):
"""
Derivative of projected fields with respect to the inversion model times a vector.
:param Source src: FDEM source
:param Mesh mesh: mesh used
:param Fields f: fields object
:param numpy.ndarray v: vector to multiply
:rtype: numpy.ndarray
:return: fields projected to recievers
"""
P = self.getP(mesh, self.projGLoc(f))
if not adjoint:
Pv_complex = P * v
Pv = getattr(Pv_complex, self.real_or_imag)
elif adjoint:
Pv_real = P.T * v
if self.real_or_imag == 'imag':
Pv = 1j*Pv_real
elif self.real_or_imag == 'real':
Pv = Pv_real.astype(complex)
else:
raise NotImplementedError('must be real or imag')
return Pv
class eField(BaseRx):
"""
Electric field FDEM receiver
:param numpy.ndarray locs: receiver locations (ie. :code:`np.r_[x,y,z]`)
:param string orientation: receiver orientation 'x', 'y' or 'z'
:param string real_or_imag: real or imaginary component 'real' or 'imag'
"""
def __init__(self, locs, orientation=None, real_or_imag=None):
self.projField = 'e'
BaseRx.__init__(self, locs, orientation, real_or_imag)
class bField(BaseRx):
"""
Magnetic flux FDEM receiver
:param numpy.ndarray locs: receiver locations (ie. :code:`np.r_[x,y,z]`)
:param string orientation: receiver orientation 'x', 'y' or 'z'
:param string real_or_imag: real or imaginary component 'real' or 'imag'
"""
def __init__(self, locs, orientation=None, real_or_imag=None):
self.projField = 'b'
BaseRx.__init__(self, locs, orientation, real_or_imag)
class hField(BaseRx):
"""
Magnetic field FDEM receiver
:param numpy.ndarray locs: receiver locations (ie. :code:`np.r_[x,y,z]`)
:param string orientation: receiver orientation 'x', 'y' or 'z'
:param string real_or_imag: real or imaginary component 'real' or 'imag'
"""
def __init__(self, locs, orientation=None, real_or_imag=None):
self.projField = 'h'
BaseRx.__init__(self, locs, orientation, real_or_imag)
class jField(BaseRx):
"""
Current density FDEM receiver
:param numpy.ndarray locs: receiver locations (ie. :code:`np.r_[x,y,z]`)
:param string orientation: receiver orientation 'x', 'y' or 'z'
:param string real_or_imag: real or imaginary component 'real' or 'imag'
"""
def __init__(self, locs, orientation=None, real_or_imag=None):
self.projField = 'j'
BaseRx.__init__(self, locs, orientation, real_or_imag)
+90 -81
View File
@@ -9,28 +9,30 @@ class BaseSrc(Survey.BaseSrc):
"""
freq = None
# rxPair = RxFDEM
integrate = True
integrate = False
def __init__(self, rxList, **kwargs):
Survey.BaseSrc.__init__(self, rxList, **kwargs)
def eval(self, prob):
"""
Evaluate the source terms.
- :math:`S_m` : magnetic source term
- :math:`S_e` : electric source term
- :math:`s_m` : magnetic source term
- :math:`s_e` : electric source term
:param Problem prob: FDEM Problem
:rtype: (numpy.ndarray, numpy.ndarray)
:return: tuple with magnetic source term and electric source term
"""
S_m = self.S_m(prob)
S_e = self.S_e(prob)
return S_m, S_e
s_m = self.s_m(prob)
s_e = self.s_e(prob)
return s_m, s_e
def evalDeriv(self, prob, v=None, adjoint=False):
"""
Derivatives of the source terms with respect to the inversion model
- :code:`S_mDeriv` : derivative of the magnetic source term
- :code:`S_eDeriv` : derivative of the electric source term
- :code:`s_mDeriv` : derivative of the magnetic source term
- :code:`s_eDeriv` : derivative of the electric source term
:param Problem prob: FDEM Problem
:param numpy.ndarray v: vector to take product with
@@ -39,9 +41,9 @@ class BaseSrc(Survey.BaseSrc):
:return: tuple with magnetic source term and electric source term derivatives times a vector
"""
if v is not None:
return self.S_mDeriv(prob, v, adjoint), self.S_eDeriv(prob, v, adjoint)
return self.s_mDeriv(prob, v, adjoint), self.s_eDeriv(prob, v, adjoint)
else:
return lambda v: self.S_mDeriv(prob, v, adjoint), lambda v: self.S_eDeriv(prob, v, adjoint)
return lambda v: self.s_mDeriv(prob, v, adjoint), lambda v: self.s_eDeriv(prob, v, adjoint)
def bPrimary(self, prob):
"""
@@ -83,7 +85,7 @@ class BaseSrc(Survey.BaseSrc):
"""
return Zero()
def S_m(self, prob):
def s_m(self, prob):
"""
Magnetic source term
@@ -93,7 +95,7 @@ class BaseSrc(Survey.BaseSrc):
"""
return Zero()
def S_e(self, prob):
def s_e(self, prob):
"""
Electric source term
@@ -103,7 +105,7 @@ class BaseSrc(Survey.BaseSrc):
"""
return Zero()
def S_mDeriv(self, prob, v, adjoint = False):
def s_mDeriv(self, prob, v, adjoint = False):
"""
Derivative of magnetic source term with respect to the inversion model
@@ -116,7 +118,7 @@ class BaseSrc(Survey.BaseSrc):
return Zero()
def S_eDeriv(self, prob, v, adjoint = False):
def s_eDeriv(self, prob, v, adjoint = False):
"""
Derivative of electric source term with respect to the inversion model
@@ -131,22 +133,21 @@ class BaseSrc(Survey.BaseSrc):
class RawVec_e(BaseSrc):
"""
RawVec electric source. It is defined by the user provided vector S_e
RawVec electric source. It is defined by the user provided vector s_e
:param list rxList: receiver list
:param float freq: frequency
:param numpy.array S_e: electric source term
:param bool integrate: Integrate the source term (multiply by Me) [True]
:param numpy.array s_e: electric source term
:param bool integrate: Integrate the source term (multiply by Me) [False]
"""
def __init__(self, rxList, freq, S_e, integrate=True): #, ePrimary=None, bPrimary=None, hPrimary=None, jPrimary=None):
self._S_e = np.array(S_e, dtype=complex)
def __init__(self, rxList, freq, s_e):
self._s_e = np.array(s_e, dtype=complex)
self.freq = float(freq)
self.integrate = integrate
BaseSrc.__init__(self, rxList)
def S_e(self, prob):
def s_e(self, prob):
"""
Electric source term
@@ -154,29 +155,28 @@ class RawVec_e(BaseSrc):
:rtype: numpy.ndarray
:return: electric source term on mesh
"""
if prob._eqLocs is 'FE' and self.integrate is True:
return prob.Me * self._S_e
return self._S_e
if prob._formulation is 'EB' and self.integrate is True:
return prob.Me * self._s_e
return self._s_e
class RawVec_m(BaseSrc):
"""
RawVec magnetic source. It is defined by the user provided vector S_m
RawVec magnetic source. It is defined by the user provided vector s_m
:param float freq: frequency
:param rxList: receiver list
:param numpy.array S_m: magnetic source term
:param bool integrate: Integrate the source term (multiply by Me) [True]
:param numpy.array s_m: magnetic source term
:param bool integrate: Integrate the source term (multiply by Me) [False]
"""
def __init__(self, rxList, freq, S_m, integrate=True): #ePrimary=Zero(), bPrimary=Zero(), hPrimary=Zero(), jPrimary=Zero()):
self._S_m = np.array(S_m, dtype=complex)
def __init__(self, rxList, freq, s_m, integrate=True): #ePrimary=Zero(), bPrimary=Zero(), hPrimary=Zero(), jPrimary=Zero()):
self._s_m = np.array(s_m, dtype=complex)
self.freq = float(freq)
self.integrate = integrate
BaseSrc.__init__(self, rxList)
def S_m(self, prob):
def s_m(self, prob):
"""
Magnetic source term
@@ -184,29 +184,28 @@ class RawVec_m(BaseSrc):
:rtype: numpy.ndarray
:return: magnetic source term on mesh
"""
if prob._eqLocs is 'EF' and self.integrate is True:
return prob.Me * self._S_m
return self._S_m
if prob._formulation is 'HJ' and self.integrate is True:
return prob.Me * self._s_m
return self._s_m
class RawVec(BaseSrc):
"""
RawVec source. It is defined by the user provided vectors S_m, S_e
RawVec source. It is defined by the user provided vectors s_m, s_e
:param rxList: receiver list
:param float freq: frequency
:param numpy.array S_m: magnetic source term
:param numpy.array S_e: electric source term
:param bool integrate: Integrate the source term (multiply by Me) [True]
:param numpy.array s_m: magnetic source term
:param numpy.array s_e: electric source term
:param bool integrate: Integrate the source term (multiply by Me) [False]
"""
def __init__(self, rxList, freq, S_m, S_e, integrate=True):
self._S_m = np.array(S_m, dtype=complex)
self._S_e = np.array(S_e, dtype=complex)
def __init__(self, rxList, freq, s_m, s_e, **kwargs):
self._s_m = np.array(s_m, dtype=complex)
self._s_e = np.array(s_e, dtype=complex)
self.freq = float(freq)
self.integrate = integrate
BaseSrc.__init__(self, rxList)
BaseSrc.__init__(self, rxList, **kwargs)
def S_m(self, prob):
def s_m(self, prob):
"""
Magnetic source term
@@ -214,11 +213,11 @@ class RawVec(BaseSrc):
:rtype: numpy.ndarray
:return: magnetic source term on mesh
"""
if prob._eqLocs is 'EF' and self.integrate is True:
return prob.Me * self._S_m
return self._S_m
if prob._formulation is 'HJ' and self.integrate is True:
return prob.Me * self._s_m
return self._s_m
def S_e(self, prob):
def s_e(self, prob):
"""
Electric source term
@@ -226,9 +225,9 @@ class RawVec(BaseSrc):
:rtype: numpy.ndarray
:return: electric source term on mesh
"""
if prob._eqLocs is 'FE' and self.integrate is True:
return prob.Me * self._S_e
return self._S_e
if prob._formulation is 'EB' and self.integrate is True:
return prob.Me * self._s_e
return self._s_e
class MagDipole(BaseSrc):
@@ -278,14 +277,13 @@ class MagDipole(BaseSrc):
:param float mu: background magnetic permeability
"""
def __init__(self, rxList, freq, loc, orientation='Z', moment=1., mu=mu_0):
def __init__(self, rxList, freq, loc, orientation='Z', moment=1., mu=mu_0, **kwargs):
self.freq = float(freq)
self.loc = loc
self.orientation = orientation
assert orientation in ['X','Y','Z'], "Orientation (right now) doesn't actually do anything! The methods in SrcUtils should take care of this..."
self.moment = moment
self.mu = mu
self.integrate = False
BaseSrc.__init__(self, rxList)
def bPrimary(self, prob):
@@ -296,15 +294,15 @@ class MagDipole(BaseSrc):
:rtype: numpy.ndarray
:return: primary magnetic field
"""
eqLocs = prob._eqLocs
formulation = prob._formulation
if eqLocs is 'FE':
if formulation is 'EB':
gridX = prob.mesh.gridEx
gridY = prob.mesh.gridEy
gridZ = prob.mesh.gridEz
C = prob.mesh.edgeCurl
elif eqLocs is 'EF':
elif formulation is 'HJ':
gridX = prob.mesh.gridFx
gridY = prob.mesh.gridFy
gridZ = prob.mesh.gridFz
@@ -335,9 +333,9 @@ class MagDipole(BaseSrc):
:return: primary magnetic field
"""
b = self.bPrimary(prob)
return h_from_b(prob,b)
return 1./self.mu * b
def S_m(self, prob):
def s_m(self, prob):
"""
The magnetic source term
@@ -347,9 +345,11 @@ class MagDipole(BaseSrc):
"""
b_p = self.bPrimary(prob)
if prob._formulation is 'HJ':
b_p = prob.Me * b_p
return -1j*omega(self.freq)*b_p
def S_e(self, prob):
def s_e(self, prob):
"""
The electric source term
@@ -361,13 +361,13 @@ class MagDipole(BaseSrc):
if all(np.r_[self.mu] == np.r_[prob.curModel.mu]):
return Zero()
else:
eqLocs = prob._eqLocs
formulation = prob._formulation
if eqLocs is 'FE':
if formulation is 'EB':
mui_s = prob.curModel.mui - 1./self.mu
MMui_s = prob.mesh.getFaceInnerProduct(mui_s)
C = prob.mesh.edgeCurl
elif eqLocs is 'EF':
elif formulation is 'HJ':
mu_s = prob.curModel.mu - self.mu
MMui_s = prob.mesh.getEdgeInnerProduct(mu_s, invMat=True)
C = prob.mesh.edgeCurl.T
@@ -410,15 +410,15 @@ class MagDipole_Bfield(BaseSrc):
:return: primary magnetic field
"""
eqLocs = prob._eqLocs
formulation = prob._formulation
if eqLocs is 'FE':
if formulation is 'EB':
gridX = prob.mesh.gridFx
gridY = prob.mesh.gridFy
gridZ = prob.mesh.gridFz
C = prob.mesh.edgeCurl
elif eqLocs is 'EF':
elif formulation is 'HJ':
gridX = prob.mesh.gridEx
gridY = prob.mesh.gridEy
gridZ = prob.mesh.gridEz
@@ -449,9 +449,9 @@ class MagDipole_Bfield(BaseSrc):
:return: primary magnetic field
"""
b = self.bPrimary(prob)
return h_from_b(prob, b)
return 1/self.mu * b
def S_m(self, prob):
def s_m(self, prob):
"""
The magnetic source term
@@ -460,9 +460,11 @@ class MagDipole_Bfield(BaseSrc):
:return: primary magnetic field
"""
b = self.bPrimary(prob)
if prob._formulation is 'HJ':
b = prob.Me * b
return -1j*omega(self.freq)*b
def S_e(self, prob):
def s_e(self, prob):
"""
The electric source term
@@ -473,13 +475,13 @@ class MagDipole_Bfield(BaseSrc):
if all(np.r_[self.mu] == np.r_[prob.curModel.mu]):
return Zero()
else:
eqLocs = prob._eqLocs
formulation = prob._formulation
if eqLocs is 'FE':
if formulation is 'EB':
mui_s = prob.curModel.mui - 1./self.mu
MMui_s = prob.mesh.getFaceInnerProduct(mui_s)
C = prob.mesh.edgeCurl
elif eqLocs is 'EF':
elif formulation is 'HJ':
mu_s = prob.curModel.mu - self.mu
MMui_s = prob.mesh.getEdgeInnerProduct(mu_s, invMat=True)
C = prob.mesh.edgeCurl.T
@@ -521,15 +523,15 @@ class CircularLoop(BaseSrc):
:rtype: numpy.ndarray
:return: primary magnetic field
"""
eqLocs = prob._eqLocs
formulation = prob._formulation
if eqLocs is 'FE':
if formulation is 'EB':
gridX = prob.mesh.gridEx
gridY = prob.mesh.gridEy
gridZ = prob.mesh.gridEz
C = prob.mesh.edgeCurl
elif eqLocs is 'EF':
elif formulation is 'HJ':
gridX = prob.mesh.gridFx
gridY = prob.mesh.gridFy
gridZ = prob.mesh.gridFz
@@ -539,7 +541,8 @@ class CircularLoop(BaseSrc):
if not prob.mesh.isSymmetric:
# TODO ?
raise NotImplementedError('Non-symmetric cyl mesh not implemented yet!')
a = MagneticLoopVectorPotential(self.loc, gridY, 'y', self.radius, mu=self.mu)
a = MagneticLoopVectorPotential(self.loc, gridY, 'y', moment=self.radius, mu=self.mu)
else:
srcfct = MagneticLoopVectorPotential
ax = srcfct(self.loc, gridX, 'x', self.radius, mu=self.mu)
@@ -560,7 +563,7 @@ class CircularLoop(BaseSrc):
b = self.bPrimary(prob)
return 1./self.mu*b
def S_m(self, prob):
def s_m(self, prob):
"""
The magnetic source term
@@ -569,9 +572,11 @@ class CircularLoop(BaseSrc):
:return: primary magnetic field
"""
b = self.bPrimary(prob)
if prob._formulation is 'HJ':
b = prob.Me * b
return -1j*omega(self.freq)*b
def S_e(self, prob):
def s_e(self, prob):
"""
The electric source term
@@ -582,13 +587,15 @@ class CircularLoop(BaseSrc):
if all(np.r_[self.mu] == np.r_[prob.curModel.mu]):
return Zero()
else:
eqLocs = prob._eqLocs
formulation = prob._formulation
if eqLocs is 'FE':
if formulation is 'EB':
mui_s = prob.curModel.mui - 1./self.mu
MMui_s = prob.mesh.getFaceInnerProduct(mui_s)
C = prob.mesh.edgeCurl
elif eqLocs is 'EF':
elif formulation is 'HJ':
mu_s = prob.curModel.mu - self.mu
MMui_s = prob.mesh.getEdgeInnerProduct(mu_s, invMat=True)
C = prob.mesh.edgeCurl.T
@@ -596,3 +603,5 @@ class CircularLoop(BaseSrc):
return -C.T * (MMui_s * self.bPrimary(prob))
+7 -132
View File
@@ -1,123 +1,13 @@
import SimPEG
from SimPEG.EM.Utils import *
from SimPEG.EM.Base import BaseEMSurvey
from scipy.constants import mu_0
from SimPEG.Utils import Zero, Identity
import SrcFDEM as Src
import RxFDEM as Rx
from SimPEG import sp
####################################################
# Receivers
####################################################
class Rx(SimPEG.Survey.BaseRx):
"""
Frequency domain receivers
:param numpy.ndarray locs: receiver locations (ie. :code:`np.r_[x,y,z]`)
:param string rxType: reciever type from knownRxTypes
"""
knownRxTypes = {
'exr':['e', 'Ex', 'real'],
'eyr':['e', 'Ey', 'real'],
'ezr':['e', 'Ez', 'real'],
'exi':['e', 'Ex', 'imag'],
'eyi':['e', 'Ey', 'imag'],
'ezi':['e', 'Ez', 'imag'],
'bxr':['b', 'Fx', 'real'],
'byr':['b', 'Fy', 'real'],
'bzr':['b', 'Fz', 'real'],
'bxi':['b', 'Fx', 'imag'],
'byi':['b', 'Fy', 'imag'],
'bzi':['b', 'Fz', 'imag'],
'jxr':['j', 'Fx', 'real'],
'jyr':['j', 'Fy', 'real'],
'jzr':['j', 'Fz', 'real'],
'jxi':['j', 'Fx', 'imag'],
'jyi':['j', 'Fy', 'imag'],
'jzi':['j', 'Fz', 'imag'],
'hxr':['h', 'Ex', 'real'],
'hyr':['h', 'Ey', 'real'],
'hzr':['h', 'Ez', 'real'],
'hxi':['h', 'Ex', 'imag'],
'hyi':['h', 'Ey', 'imag'],
'hzi':['h', 'Ez', 'imag'],
}
radius = None
def __init__(self, locs, rxType):
SimPEG.Survey.BaseRx.__init__(self, locs, rxType)
@property
def projField(self):
"""Field Type projection (e.g. e b ...)"""
return self.knownRxTypes[self.rxType][0]
@property
def projGLoc(self):
"""Grid Location projection (e.g. Ex Fy ...)"""
return self.knownRxTypes[self.rxType][1]
@property
def projComp(self):
"""Component projection (real/imag)"""
return self.knownRxTypes[self.rxType][2]
def eval(self, src, mesh, f):
"""
Project fields to recievers to get data.
:param Source src: FDEM source
:param Mesh mesh: mesh used
:param Fields f: fields object
:rtype: numpy.ndarray
:return: fields projected to recievers
"""
P = self.getP(mesh) # get interpolation to recievers
u_part_complex = f[src, self.projField]
real_or_imag = self.projComp # get the real or imag component
u_part = getattr(u_part_complex, real_or_imag)
return P*u_part
def evalDeriv(self, src, mesh, f, v, adjoint=False):
"""
Derivative of projected fields with respect to the inversion model times a vector.
:param Source src: FDEM source
:param Mesh mesh: mesh used
:param Fields f: fields object
:param numpy.ndarray v: vector to multiply
:rtype: numpy.ndarray
:return: fields projected to recievers
"""
P = self.getP(mesh)
if not adjoint:
Pv_complex = P * v
real_or_imag = self.projComp
Pv = getattr(Pv_complex, real_or_imag)
elif adjoint:
Pv_real = P.T * v
real_or_imag = self.projComp
if real_or_imag == 'imag':
Pv = 1j*Pv_real
elif real_or_imag == 'real':
Pv = Pv_real.astype(complex)
else:
raise NotImplementedError('must be real or imag')
return Pv
####################################################
# Survey
####################################################
class Survey(SimPEG.Survey.BaseSurvey):
class Survey(BaseEMSurvey):
"""
Frequency domain electromagnetic survey
@@ -125,12 +15,12 @@ class Survey(SimPEG.Survey.BaseSurvey):
"""
srcPair = Src.BaseSrc
rxPair = Rx
rxPair = Rx.BaseRx
def __init__(self, srcList, **kwargs):
# Sort these by frequency
self.srcList = srcList
SimPEG.Survey.BaseSurvey.__init__(self, **kwargs)
BaseEMSurvey.__init__(self, srcList, **kwargs)
_freqDict = {}
for src in srcList:
@@ -165,23 +55,8 @@ class Survey(SimPEG.Survey.BaseSurvey):
Returns the sources associated with a specific frequency.
:param float freq: frequency for which we look up sources
:rtype: dictionary
:return: sources at the sepcified frequency
:return: sources at the sepcified frequency
"""
assert freq in self._freqDict, "The requested frequency is not in this survey."
return self._freqDict[freq]
def eval(self, u):
"""
Project fields to receiver locations
:param Fields u: fields object
:rtype: numpy.ndarray
:return: data
"""
data = SimPEG.Survey.Data(self)
for src in self.srcList:
for rx in src.rxList:
data[src, rx] = rx.eval(src, self.mesh, u)
return data
def evalDeriv(self, u):
raise Exception('Use Receivers to project fields deriv.')
+5 -3
View File
@@ -1,3 +1,5 @@
from SurveyFDEM import Rx, Src, Survey
from FDEM import BaseFDEMProblem, Problem_e, Problem_b, Problem_j, Problem_h
from FieldsFDEM import *
from SurveyFDEM import Survey
import SrcFDEM as Src
import RxFDEM as Rx
from FDEM import Problem3D_e, Problem3D_b, Problem3D_j, Problem3D_h
from FieldsFDEM import Fields3D_e, Fields3D_b, Fields3D_j, Fields3D_h
+12 -11
View File
@@ -27,6 +27,7 @@ class FieldsTDEM(Problem.TimeFields):
else:
e = np.zeros((nE,nSrc)) # if nSrc == 1 else (nE, nSrc))
u = np.concatenate((u, b, e))
return Utils.mkvc(u,nSrc)
@@ -107,11 +108,11 @@ class BaseTDEMProblem(BaseTimeProblem, BaseEMProblem):
Ainv.clean()
return F
def Jvec(self, m, v, u=None):
def Jvec(self, m, v, f=None):
"""
:param numpy.array m: Conductivity model
:param numpy.ndarray v: vector (model object)
:param simpegEM.TDEM.FieldsTDEM u: Fields resulting from m
:param simpegEM.TDEM.FieldsTDEM f: Fields resulting from m
:rtype: numpy.ndarray
:return: w (data object)
@@ -124,15 +125,15 @@ class BaseTDEMProblem(BaseTimeProblem, BaseEMProblem):
"""
if self.verbose: print '%s\nCalculating J(v)\n%s'%('*'*50,'*'*50)
self.curModel = m
if u is None:
u = self.fields(m)
p = self.Gvec(m, v, u)
if f is None:
f = self.fields(m)
p = self.Gvec(m, v, f)
y = self.solveAh(m, p)
Jv = self.survey.evalDeriv(u, v=y)
Jv = self.survey.evalDeriv(f, v=y)
if self.verbose: print '%s\nDone calculating J(v)\n%s'%('*'*50,'*'*50)
return - mkvc(Jv)
def Jtvec(self, m, v, u=None):
def Jtvec(self, m, v, f=None):
"""
:param numpy.array m: Conductivity model
:param numpy.ndarray,SimPEG.Survey.Data v: vector (data object)
@@ -149,15 +150,15 @@ class BaseTDEMProblem(BaseTimeProblem, BaseEMProblem):
"""
if self.verbose: print '%s\nCalculating J^T(v)\n%s'%('*'*50,'*'*50)
self.curModel = m
if u is None:
u = self.fields(m)
if f is None:
f = self.fields(m)
if not isinstance(v, self.dataPair):
v = self.dataPair(self.survey, v)
p = self.survey.evalDeriv(u, v=v, adjoint=True)
p = self.survey.evalDeriv(f, v=v, adjoint=True)
y = self.solveAht(m, p)
w = self.Gtvec(m, y, u)
w = self.Gtvec(m, y, f)
if self.verbose: print '%s\nDone calculating J^T(v)\n%s'%('*'*50,'*'*50)
return - mkvc(w)
-33
View File
@@ -13,37 +13,4 @@ def k(freq, sigma, mu=mu_0, eps=epsilon_0):
beta = w * np.sqrt( mu*eps/2 * ( np.sqrt(1. + (sigma / (eps*w))**2 ) - 1) )
return alp - 1j*beta
# Constitutive relations
def e_from_j(prob,j):
eqLocs = prob._eqLocs
if eqLocs is 'FE':
MSigmaI = prob.MeSigmaI
elif eqLocs is 'EF':
MSigmaI = prob.MfRho
return MSigmaI*j
def j_from_e(prob,e):
eqLocs = prob._eqLocs
if eqLocs is 'FE':
MSigma = prob.MeSigma
elif eqLocs is 'EF':
MSigma = prob.MfRhoI
return MSigma*e
def b_from_h(prob,h):
eqLocs = prob._eqLocs
if eqLocs is 'FE':
MMu = prob.MfMuiI
elif eqLocs is 'EF':
MMu = prob.MeMu
return MMu*h
def h_from_b(prob,b):
eqLocs = prob._eqLocs
if eqLocs is 'FE':
MMuI = prob.MfMui
elif eqLocs is 'EF':
MMuI = prob.MeMuI
return MMuI*b
+1 -4
View File
@@ -1,5 +1,2 @@
# import Sources
# import Ana
# import Solver
from EMUtils import omega, e_from_j, j_from_e, b_from_h, h_from_b
from EMUtils import omega, k
from AnalyticUtils import MagneticDipoleFields, MagneticDipoleVectorPotential, MagneticLoopVectorPotential
+79 -23
View File
@@ -4,63 +4,77 @@ from SimPEG import EM
import sys
from scipy.constants import mu_0
def getFDEMProblem(fdemType, comp, SrcList, freq, verbose=False):
cs = 5.
ncx, ncy, ncz = 6, 6, 6
npad = 3
FLR = 1e-20 # "zero", so if residual below this --> pass regardless of order
CONDUCTIVITY = 1e1
MU = mu_0
freq = 5e-1
def getFDEMProblem(fdemType, comp, SrcList, freq, useMu=False, verbose=False):
cs = 10.
ncx, ncy, ncz = 0, 0, 0
npad = 8
hx = [(cs,npad,-1.3), (cs,ncx), (cs,npad,1.3)]
hy = [(cs,npad,-1.3), (cs,ncy), (cs,npad,1.3)]
hz = [(cs,npad,-1.3), (cs,ncz), (cs,npad,1.3)]
mesh = Mesh.TensorMesh([hx,hy,hz],['C','C','C'])
mapping = Maps.ExpMap(mesh)
if useMu is True:
mapping = [('sigma', Maps.ExpMap(mesh)), ('mu', Maps.IdentityMap(mesh))]
else:
mapping = Maps.ExpMap(mesh)
x = np.array([np.linspace(-30,-15,3),np.linspace(15,30,3)]) #don't sample right by the source
XYZ = Utils.ndgrid(x,x,np.r_[0.])
Rx0 = EM.FDEM.Rx(XYZ, comp)
x = np.array([np.linspace(-5.*cs,-2.*cs,3),np.linspace(5.*cs,2.*cs,3)]) + cs/4. #don't sample right by the source, slightly off alignment from either staggered grid
XYZ = Utils.ndgrid(x,x,np.linspace(-2.*cs,2.*cs,5))
Rx0 = getattr(EM.FDEM.Rx, comp[0] + 'Field')
if comp[2] == 'r':
real_or_imag = 'real'
elif comp[2] == 'i':
real_or_imag = 'imag'
rx0 = Rx0(XYZ, comp[1], 'imag')
Src = []
for SrcType in SrcList:
if SrcType is 'MagDipole':
Src.append(EM.FDEM.Src.MagDipole([Rx0], freq=freq, loc=np.r_[0.,0.,0.]))
Src.append(EM.FDEM.Src.MagDipole([rx0], freq=freq, loc=np.r_[0.,0.,0.]))
elif SrcType is 'MagDipole_Bfield':
Src.append(EM.FDEM.Src.MagDipole_Bfield([Rx0], freq=freq, loc=np.r_[0.,0.,0.]))
Src.append(EM.FDEM.Src.MagDipole_Bfield([rx0], freq=freq, loc=np.r_[0.,0.,0.]))
elif SrcType is 'CircularLoop':
Src.append(EM.FDEM.Src.CircularLoop([Rx0], freq=freq, loc=np.r_[0.,0.,0.]))
Src.append(EM.FDEM.Src.CircularLoop([rx0], freq=freq, loc=np.r_[0.,0.,0.]))
elif SrcType is 'RawVec':
if fdemType is 'e' or fdemType is 'b':
S_m = np.zeros(mesh.nF)
S_e = np.zeros(mesh.nE)
S_m[Utils.closestPoints(mesh,[0.,0.,0.],'Fz') + np.sum(mesh.vnF[:1])] = 1.
S_e[Utils.closestPoints(mesh,[0.,0.,0.],'Ez') + np.sum(mesh.vnE[:1])] = 1.
Src.append(EM.FDEM.Src.RawVec([Rx0], freq, S_m, S_e))
S_m[Utils.closestPoints(mesh,[0.,0.,0.],'Fz') + np.sum(mesh.vnF[:1])] = 1e-3
S_e[Utils.closestPoints(mesh,[0.,0.,0.],'Ez') + np.sum(mesh.vnE[:1])] = 1e-3
Src.append(EM.FDEM.Src.RawVec([rx0], freq, S_m, mesh.getEdgeInnerProduct()*S_e))
elif fdemType is 'h' or fdemType is 'j':
S_m = np.zeros(mesh.nE)
S_e = np.zeros(mesh.nF)
S_m[Utils.closestPoints(mesh,[0.,0.,0.],'Ez') + np.sum(mesh.vnE[:1])] = 1.
S_e[Utils.closestPoints(mesh,[0.,0.,0.],'Fz') + np.sum(mesh.vnF[:1])] = 1.
Src.append(EM.FDEM.Src.RawVec([Rx0], freq, S_m, S_e))
S_m[Utils.closestPoints(mesh,[0.,0.,0.],'Ez') + np.sum(mesh.vnE[:1])] = 1e-3
S_e[Utils.closestPoints(mesh,[0.,0.,0.],'Fz') + np.sum(mesh.vnF[:1])] = 1e-3
Src.append(EM.FDEM.Src.RawVec([rx0], freq, mesh.getEdgeInnerProduct()*S_m, S_e))
if verbose:
print ' Fetching %s problem' % (fdemType)
if fdemType == 'e':
survey = EM.FDEM.Survey(Src)
prb = EM.FDEM.Problem_e(mesh, mapping=mapping)
prb = EM.FDEM.Problem3D_e(mesh, mapping=mapping)
elif fdemType == 'b':
survey = EM.FDEM.Survey(Src)
prb = EM.FDEM.Problem_b(mesh, mapping=mapping)
prb = EM.FDEM.Problem3D_b(mesh, mapping=mapping)
elif fdemType == 'j':
survey = EM.FDEM.Survey(Src)
prb = EM.FDEM.Problem_j(mesh, mapping=mapping)
prb = EM.FDEM.Problem3D_j(mesh, mapping=mapping)
elif fdemType == 'h':
survey = EM.FDEM.Survey(Src)
prb = EM.FDEM.Problem_h(mesh, mapping=mapping)
prb = EM.FDEM.Problem3D_h(mesh, mapping=mapping)
else:
raise NotImplementedError()
@@ -70,6 +84,48 @@ def getFDEMProblem(fdemType, comp, SrcList, freq, verbose=False):
from pymatsolver import MumpsSolver
prb.Solver = MumpsSolver
except ImportError, e:
pass
prb.Solver = SolverLU
return prb
return prb
def crossCheckTest(SrcList, fdemType1, fdemType2, comp, addrandoms = False, useMu=False, TOL=1e-5, verbose=False):
l2norm = lambda r: np.sqrt(r.dot(r))
prb1 = getFDEMProblem(fdemType1, comp, SrcList, freq, useMu, verbose)
mesh = prb1.mesh
print 'Cross Checking Forward: %s, %s formulations - %s' % (fdemType1, fdemType2, comp)
logsig = np.log(np.ones(mesh.nC)*CONDUCTIVITY)
mu = np.ones(mesh.nC)*MU
if addrandoms is True:
logsig += np.random.randn(mesh.nC)*np.log(CONDUCTIVITY)*1e-1
mu += np.random.randn(mesh.nC)*MU*1e-1
if useMu is True:
m = np.r_[logsig, mu]
else:
m = logsig
survey1 = prb1.survey
d1 = survey1.dpred(m)
if verbose:
print ' Problem 1 solved'
prb2 = getFDEMProblem(fdemType2, comp, SrcList, freq, useMu, verbose)
survey2 = prb2.survey
d2 = survey2.dpred(m)
if verbose:
print ' Problem 2 solved'
r = d2-d1
l2r = l2norm(r)
tol = np.max([TOL*(10**int(np.log10(0.5* (l2norm(d1) + l2norm(d2)) ))),FLR])
print l2norm(d1), l2norm(d2), l2r , tol, l2r < tol
return l2r < tol
+68
View File
@@ -0,0 +1,68 @@
from SimPEG import *
import SimPEG.DCIP as DC
def run(plotIt=False):
cs = 25.
hx = [(cs,7, -1.3),(cs,21),(cs,7, 1.3)]
hy = [(cs,7, -1.3),(cs,21),(cs,7, 1.3)]
hz = [(cs,7, -1.3),(cs,20)]
mesh = Mesh.TensorMesh([hx, hy, hz], 'CCN')
sighalf = 1e-2
sigma = np.ones(mesh.nC)*sighalf
xtemp = np.linspace(-150, 150, 21)
ytemp = np.linspace(-150, 150, 21)
xyz_rxP = Utils.ndgrid(xtemp-10., ytemp, np.r_[0.])
xyz_rxN = Utils.ndgrid(xtemp+10., ytemp, np.r_[0.])
xyz_rxM = Utils.ndgrid(xtemp, ytemp, np.r_[0.])
# if plotIt:
# fig, ax = plt.subplots(1,1, figsize = (5,5))
# mesh.plotSlice(sigma, grid=True, ax = ax)
# ax.plot(xyz_rxP[:,0],xyz_rxP[:,1], 'w.')
# ax.plot(xyz_rxN[:,0],xyz_rxN[:,1], 'r.', ms = 3)
rx = DC.RxDipole(xyz_rxP, xyz_rxN)
src = DC.SrcDipole([rx], [-200, 0, -12.5], [+200, 0, -12.5])
survey = DC.SurveyDC([src])
problem = DC.ProblemDC_CC(mesh)
problem.pair(survey)
try:
from pymatsolver import MumpsSolver
problem.Solver = MumpsSolver
except Exception, e:
pass
data = survey.dpred(sigma)
def DChalf(srclocP, srclocN, rxloc, sigma, I=1.):
rp = (srclocP.reshape([1,-1])).repeat(rxloc.shape[0], axis = 0)
rn = (srclocN.reshape([1,-1])).repeat(rxloc.shape[0], axis = 0)
rP = np.sqrt(((rxloc-rp)**2).sum(axis=1))
rN = np.sqrt(((rxloc-rn)**2).sum(axis=1))
return I/(sigma*2.*np.pi)*(1/rP-1/rN)
data_anaP = DChalf(np.r_[-200, 0, 0.],np.r_[+200, 0, 0.], xyz_rxP, sighalf)
data_anaN = DChalf(np.r_[-200, 0, 0.],np.r_[+200, 0, 0.], xyz_rxN, sighalf)
data_ana = data_anaP-data_anaN
Data_ana = data_ana.reshape((21, 21), order = 'F')
Data = data.reshape((21, 21), order = 'F')
X = xyz_rxM[:,0].reshape((21, 21), order = 'F')
Y = xyz_rxM[:,1].reshape((21, 21), order = 'F')
if plotIt:
import matplotlib.pyplot as plt
fig, ax = plt.subplots(1,2, figsize = (12, 5))
vmin = np.r_[data, data_ana].min()
vmax = np.r_[data, data_ana].max()
dat1 = ax[1].contourf(X, Y, Data, 60, vmin = vmin, vmax = vmax)
dat0 = ax[0].contourf(X, Y, Data_ana, 60, vmin = vmin, vmax = vmax)
cb0 = plt.colorbar(dat1, orientation = 'horizontal', ax = ax[0])
cb1 = plt.colorbar(dat1, orientation = 'horizontal', ax = ax[1])
ax[1].set_title('Analytic')
ax[0].set_title('Computed')
plt.show()
return np.linalg.norm(data-data_ana)/np.linalg.norm(data_ana)
if __name__ == '__main__':
print run(plotIt=True)
+210
View File
@@ -0,0 +1,210 @@
from SimPEG import Mesh, Utils, np, sp
import SimPEG.DCIP as DC
import time
def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', plotIt=True):
"""
DC Forward Simulation
=====================
Forward model two conductive spheres in a half-space and plot a
pseudo-section. Assumes an infinite line source and measures along the
center of the spheres.
INPUT:
loc = Location of spheres [[x1,y1,z1],[x2,y2,z2]]
radi = Radius of spheres [r1,r2]
param = Conductivity of background and two spheres [m0,m1,m2]
stype = survey type "pdp" (pole dipole) or "dpdp" (dipole dipole)
dtype = Data type "appr" (app res) | "appc" (app cond) | "volt" (potential)
Created by @fourndo
"""
assert stype in ['pdp', 'dpdp'], "Source type (stype) must be pdp or dpdp (pole dipole or dipole dipole)"
assert dtype in ['appr', 'appc', 'volt'], "Data type (dtype) must be appr (app res) or appc (app cond) or volt (potential)"
if loc is None:
loc = np.c_[[-50.,0.,-50.],[50.,0.,-50.]]
if sig is None:
sig = np.r_[1e-2,1e-1,1e-3]
if radi is None:
radi = np.r_[25.,25.]
if param is None:
param = np.r_[30.,30.,5]
# First we need to create a mesh and a model.
# This is our mesh
dx = 5.
hxind = [(dx,15,-1.3), (dx, 75), (dx,15,1.3)]
hyind = [(dx,15,-1.3), (dx, 10), (dx,15,1.3)]
hzind = [(dx,15,-1.3),(dx, 15)]
mesh = Mesh.TensorMesh([hxind, hyind, hzind], 'CCN')
# Set background conductivity
model = np.ones(mesh.nC) * sig[0]
# First anomaly
ind = Utils.ModelBuilder.getIndicesSphere(loc[:,0],radi[0],mesh.gridCC)
model[ind] = sig[1]
# Second anomaly
ind = Utils.ModelBuilder.getIndicesSphere(loc[:,1],radi[1],mesh.gridCC)
model[ind] = sig[2]
# Get index of the center
indy = int(mesh.nCy/2)
# Plot the model for reference
# Define core mesh extent
xlim = 200
zlim = 100
# Then specify the end points of the survey. Let's keep it simple for now and survey above the anomalies, top of the mesh
ends = [(-175,0),(175,0)]
ends = np.c_[np.asarray(ends),np.ones(2).T*mesh.vectorNz[-1]]
# Snap the endpoints to the grid. Easier to create 2D section.
indx = Utils.closestPoints(mesh, ends )
locs = np.c_[mesh.gridCC[indx,0],mesh.gridCC[indx,1],np.ones(2).T*mesh.vectorNz[-1]]
# We will handle the geometry of the survey for you and create all the combination of tx-rx along line
# [Tx, Rx] = DC.gen_DCIPsurvey(locs, mesh, stype, param[0], param[1], param[2])
survey, Tx, Rx = DC.gen_DCIPsurvey(locs, mesh, stype, param[0], param[1], param[2])
# Define some global geometry
dl_len = np.sqrt( np.sum((locs[0,:] - locs[1,:])**2) )
dl_x = ( Tx[-1][0,1] - Tx[0][0,0] ) / dl_len
dl_y = ( Tx[-1][1,1] - Tx[0][1,0] ) / dl_len
#azm = np.arctan(dl_y/dl_x)
#Set boundary conditions
mesh.setCellGradBC('neumann')
# Define the linear system needed for the DC problem. We assume an infitite
# line source for simplicity.
Div = mesh.faceDiv
Grad = mesh.cellGrad
Msig = Utils.sdiag(1./(mesh.aveF2CC.T*(1./model)))
A = Div*Msig*Grad
# Change one corner to deal with nullspace
A[0,0] = 1
A = sp.csc_matrix(A)
# We will solve the system iteratively, so a pre-conditioner is helpful
# This is simply a Jacobi preconditioner (inverse of the main diagonal)
dA = A.diagonal()
P = sp.spdiags(1/dA,0,A.shape[0],A.shape[0])
# Now we can solve the system for all the transmitters
# We want to store the data
data = []
# There is probably a more elegant way to do this, but we can just for-loop through the transmitters
for ii in range(len(Tx)):
start_time = time.time() # Let's time the calculations
#print("Transmitter %i / %i\r" % (ii+1,len(Tx)))
# Select dipole locations for receiver
rxloc_M = np.asarray(Rx[ii][:,0:3])
rxloc_N = np.asarray(Rx[ii][:,3:])
# For usual cases "dpdp" or "gradient"
if stype == 'pdp':
# Create an "inifinity" pole
tx = np.squeeze(Tx[ii][:,0:1])
tinf = tx + np.array([dl_x,dl_y,0])*dl_len*2
inds = Utils.closestPoints(mesh, np.c_[tx,tinf].T)
RHS = mesh.getInterpolationMat(np.asarray(Tx[ii]).T, 'CC').T*( [-1] / mesh.vol[inds] )
else:
inds = Utils.closestPoints(mesh, np.asarray(Tx[ii]).T )
RHS = mesh.getInterpolationMat(np.asarray(Tx[ii]).T, 'CC').T*( [-1,1] / mesh.vol[inds] )
# Iterative Solve
Ainvb = sp.linalg.bicgstab(P*A,P*RHS, tol=1e-5)
# We now have the potential everywhere
phi = Utils.mkvc(Ainvb[0])
# Solve for phi on pole locations
P1 = mesh.getInterpolationMat(rxloc_M, 'CC')
P2 = mesh.getInterpolationMat(rxloc_N, 'CC')
# Compute the potential difference
dtemp = (P1*phi - P2*phi)*np.pi
data.append( dtemp )
print '\rTransmitter {0} of {1} -> Time:{2} sec'.format(ii,len(Tx),time.time()- start_time),
print 'Transmitter {0} of {1}'.format(ii,len(Tx))
print 'Forward completed'
# Let's just convert the 3D format into 2D (distance along line) and plot
survey2D = DC.convertObs_DC3D_to_2D(survey, np.ones(survey.nSrc) , 'Xloc')
survey2D.dobs =np.hstack(data)
if plotIt:
import matplotlib.pyplot as plt
fig = plt.figure(figsize=(7,7))
ax = plt.subplot(2,1,1, aspect='equal')
# Plot the location of the spheres for reference
circle1=plt.Circle((loc[0,0],loc[2,0]),radi[0],color='w',fill=False, lw=3)
circle2=plt.Circle((loc[0,1],loc[2,1]),radi[1],color='k',fill=False, lw=3)
ax.add_artist(circle1)
ax.add_artist(circle2)
dat = mesh.plotSlice(np.log10(model), ax =ax, normal = 'Y',
ind = indy,grid=True, clim = np.log10([sig.min(),sig.max()]))
ax.set_title('3-D model')
plt.gca().set_aspect('equal', adjustable='box')
plt.scatter(Tx[0][0,:],Tx[0][2,:],s=40,c='g', marker='v')
plt.scatter(Rx[0][:,0::3],Rx[0][:,2::3],s=40,c='y')
plt.xlim([-xlim,xlim])
plt.ylim([-zlim,mesh.vectorNz[-1]+dx])
pos = ax.get_position()
ax.set_position([pos.x0 , pos.y0 + 0.025 , pos.width, pos.height])
pos = ax.get_position()
cbarax = fig.add_axes([pos.x0 , pos.y0 + 0.025 , pos.width, pos.height * 0.04]) ## the parameters are the specified position you set
cb = fig.colorbar(dat[0],cax=cbarax, orientation="horizontal",
ax = ax, ticks=np.linspace(np.log10(sig.min()),
np.log10(sig.max()), 3), format="$10^{%.1f}$")
cb.set_label("Conductivity (S/m)",size=12)
cb.ax.tick_params(labelsize=12)
# Second plot for the predicted apparent resistivity data
ax2 = plt.subplot(2,1,2, aspect='equal')
# Plot the location of the spheres for reference
circle1=plt.Circle((loc[0,0],loc[2,0]),radi[0],color='w',fill=False, lw=3)
circle2=plt.Circle((loc[0,1],loc[2,1]),radi[1],color='k',fill=False, lw=3)
ax2.add_artist(circle1)
ax2.add_artist(circle2)
# Add the speudo section
dat = DC.plot_pseudoSection(survey2D,ax2,stype=stype, dtype = dtype)
# plt.scatter(Tx2d[0][:],Tx[0][2,:],s=40,c='g', marker='v')
# plt.scatter(Rx2d[0][:],Rx[0][:,2::3],s=40,c='y')
# plt.plot(np.r_[Tx2d[0][0],Rx2d[-1][-1,-1]],np.ones(2)*mesh.vectorNz[-1], color='k')
ax2.set_title('Apparent Conductivity data')
plt.ylim([-zlim,mesh.vectorNz[-1]+dx])
plt.show()
return fig, ax
if __name__ == '__main__':
run()
+3 -4
View File
@@ -43,16 +43,15 @@ def run(plotIt=True):
rxOffset=10.
bzi = EM.FDEM.Rx(np.array([[rxOffset, 0., 1e-3]]), 'bzi')
bzi = EM.FDEM.Rx.bField(np.array([[rxOffset, 0., 1e-3]]), orientation='z', real_or_imag='imag')
freqs = np.logspace(1,3,10)
srcLoc = np.array([0., 0., 10.])
srcList = []
[srcList.append(EM.FDEM.Src.MagDipole([bzi],freq, srcLoc,orientation='Z')) for freq in freqs]
srcList = [EM.FDEM.Src.MagDipole([bzi],freq, srcLoc,orientation='Z') for freq in freqs]
survey = EM.FDEM.Survey(srcList)
prb = EM.FDEM.Problem_b(mesh, mapping=mapping)
prb = EM.FDEM.Problem3D_b(mesh, mapping=mapping)
try:
from pymatsolver import MumpsSolver
@@ -0,0 +1,275 @@
from SimPEG import *
from SimPEG.EM import FDEM, Analytics, mu_0
import time
try:
from pymatsolver import MumpsSolver
solver = MumpsSolver
except Exception:
solver = SolverLU
pass
def run(plotIt=True):
"""
EM: Schenkel and Morrison Casing Model
======================================
Here we create and run a FDEM forward simulation to calculate the vertical
current inside a steel-cased. The model is based on the Schenkel and
Morrison Casing Model, and the results are used in a 2016 SEG abstract by
Yang et al.
- Schenkel, C.J., and H.F. Morrison, 1990, Effects of well casing on potential field measurements using downhole current sources: Geophysical prospecting, 38, 663-686.
The model consists of:
- Air: Conductivity 1e-8 S/m, above z = 0
- Background: conductivity 1e-2 S/m, below z = 0
- Casing: conductivity 1e6 S/m
- 300m long
- radius of 0.1m
- thickness of 6e-3m
Inside the casing, we take the same conductivity as the background.
We are using an EM code to simulate DC, so we use frequency low enough
that the skin depth inside the casing is longer than the casing length (f
= 1e-6 Hz). The plot produced is of the current inside the casing.
These results are shown in the SEG abstract by Yang et al., 2016: 3D DC
resistivity modeling of steel casing for reservoir monitoring using
equivalent resistor network. The solver used to produce these results and
achieve the CPU time of ~30s is Mumps, which was installed using pymatsolver_
.. _pymatsolver: https://github.com/rowanc1/pymatsolver
This example is on figshare: https://dx.doi.org/10.6084/m9.figshare.3126961.v1
If you would use this example for a code comparison, or build upon it, a
citation would be much appreciated!
"""
if plotIt:
import matplotlib.pylab as plt
# ------------------ MODEL ------------------
sigmaair = 1e-8 # air
sigmaback = 1e-2 # background
sigmacasing = 1e6 # casing
sigmainside = sigmaback # inside the casing
casing_t = 0.006 # 1cm thickness
casing_l = 300 # length of the casing
casing_r = 0.1
casing_a = casing_r - casing_t/2. # inner radius
casing_b = casing_r + casing_t/2. # outer radius
casing_z = np.r_[-casing_l,0.]
# ------------------ SURVEY PARAMETERS ------------------
freqs = np.r_[1e-6] #[1e-1, 1, 5] # frequencies
dsz = -300 # down-hole z source location
src_loc = np.r_[0.,0.,dsz]
inf_loc = np.r_[0.,0.,1e4]
print 'Skin Depth: ', [(500./np.sqrt(sigmaback*_)) for _ in freqs]
# ------------------ MESH ------------------
# fine cells near well bore
csx1, csx2 = 2e-3, 60.
pfx1, pfx2 = 1.3, 1.3
ncx1 = np.ceil(casing_b/csx1+2)
# pad nicely to second cell size
npadx1 = np.floor(np.log(csx2/csx1) / np.log(pfx1))
hx1a,hx1b = Utils.meshTensor([(csx1,ncx1)]),Utils.meshTensor([(csx1,npadx1,pfx1)])
dx1 = sum(hx1a)+sum(hx1b)
dx1 = np.floor(dx1/csx2)
hx1b *= (dx1*csx2 - sum(hx1a))/sum(hx1b)
# second chunk of mesh
dx2 = 300. # uniform mesh out to here
ncx2 = np.ceil((dx2 - dx1)/csx2)
npadx2 = 45
hx2a, hx2b = Utils.meshTensor([(csx2,ncx2)]), Utils.meshTensor([(csx2,npadx2,pfx2)])
hx = np.hstack([hx1a,hx1b,hx2a,hx2b])
# z-direction
csz = 0.05
nza = 10
ncz, npadzu, npadzd = np.int(np.ceil(np.diff(casing_z)[0]/csz))+10, 68, 68 # cell size, number of core cells, number of padding cells in the x- direction
hz = Utils.meshTensor([(csz,npadzd,-1.3), (csz,ncz), (csz,npadzu,1.3)]) # vector of cell widths in the z-direction
# Mesh
mesh = Mesh.CylMesh([hx,1.,hz], [0.,0.,-np.sum(hz[:npadzu+ncz-nza])])
print 'Mesh Extent xmax: %f,: zmin: %f, zmax: %f'%(mesh.vectorCCx.max(), mesh.vectorCCz.min(), mesh.vectorCCz.max())
print 'Number of cells', mesh.nC
if plotIt is True:
fig, ax = plt.subplots(1, 1, figsize=(6, 4))
ax.set_title('Simulation Mesh')
mesh.plotGrid(ax=ax)
plt.show()
# Put the model on the mesh
sigWholespace = sigmaback*np.ones((mesh.nC))
sigBack = sigWholespace.copy()
sigBack[mesh.gridCC[:,2] > 0.] = sigmaair
sigCasing = sigBack.copy()
iCasingZ = (mesh.gridCC[:,2] <= casing_z[1]) & (mesh.gridCC[:,2] >= casing_z[0])
iCasingX = (mesh.gridCC[:,0] >= casing_a) & (mesh.gridCC[:,0] <= casing_b)
iCasing = iCasingX & iCasingZ
sigCasing[iCasing] = sigmacasing
if plotIt is True:
# plotting parameters
xlim = np.r_[0., 0.2]
zlim = np.r_[-350., 10.]
clim_sig = np.r_[-8,6]
# plot models
fig, ax = plt.subplots(1,1,figsize=(4,4))
f = plt.colorbar(mesh.plotImage(np.log10(sigCasing),ax=ax)[0], ax=ax)
ax.grid(which='both')
ax.set_title('Log_10 (Sigma)')
ax.set_xlim(xlim)
ax.set_ylim(zlim)
f.set_clim(clim_sig)
plt.show()
# -------------- Sources --------------------
# Define Custom Current Sources
# surface source
sg_x = np.zeros(mesh.vnF[0],dtype=complex)
sg_y = np.zeros(mesh.vnF[1],dtype=complex)
sg_z = np.zeros(mesh.vnF[2],dtype=complex)
nza = 2 # put the wire two cells above the surface
ncin = 2
# vertically directed wire
sgv_indx = (mesh.gridFz[:,0] > casing_a) & (mesh.gridFz[:,0] < casing_a + csx1) # hook it up to casing at the surface
sgv_indz = (mesh.gridFz[:,2] <= +csz*nza) & (mesh.gridFz[:,2] >= -csz*2)
sgv_ind = sgv_indx & sgv_indz
sg_z[sgv_ind] = -1.
# horizontally directed wire
sgh_indx = (mesh.gridFx[:,0] > casing_a) & (mesh.gridFx[:,0] <= inf_loc[2])
sgh_indz = (mesh.gridFx[:,2] > csz*(nza-0.5)) & (mesh.gridFx[:,2] < csz*(nza+0.5))
sgh_ind = sgh_indx & sgh_indz
sg_x[sgh_ind] = -1.
sgv2_indx = (mesh.gridFz[:,0] >= mesh.gridFx[sgh_ind,0].max()) & (mesh.gridFz[:,0] <= inf_loc[2]*1.2) # hook it up to casing at the surface
sgv2_indz = (mesh.gridFz[:,2] <= +csz*nza) & (mesh.gridFz[:,2] >= -csz*2)
sgv2_ind = sgv2_indx & sgv2_indz
sg_z[sgv2_ind] = 1.
# assemble the source
sg = np.hstack([sg_x,sg_y,sg_z])
sg_p = [FDEM.Src.RawVec_e([],_,sg/mesh.area) for _ in freqs]
# downhole source
dg_x = np.zeros(mesh.vnF[0],dtype=complex)
dg_y = np.zeros(mesh.vnF[1],dtype=complex)
dg_z = np.zeros(mesh.vnF[2],dtype=complex)
# vertically directed wire
dgv_indx = (mesh.gridFz[:,0] < csx1) # go through the center of the well
dgv_indz = (mesh.gridFz[:,2] <= +csz*nza) & (mesh.gridFz[:,2] > dsz + csz/2.)
dgv_ind = dgv_indx & dgv_indz
dg_z[dgv_ind] = -1.
# couple to the casing downhole
dgh_indx = mesh.gridFx[:,0] < casing_a + csx1
dgh_indz = (mesh.gridFx[:,2] < dsz + csz) & (mesh.gridFx[:,2] >= dsz)
dgh_ind = dgh_indx & dgh_indz
dg_x[dgh_ind] = 1.
# horizontal part at surface
dgh2_indx = mesh.gridFx[:,0] <= inf_loc[2]*1.2
dgh2_indz = sgh_indz.copy()
dgh2_ind = dgh2_indx & dgh2_indz
dg_x[dgh2_ind] = -1.
# vertical part at surface
dgv2_ind = sgv2_ind.copy()
dg_z[dgv2_ind] = 1.
# assemble the source
dg = np.hstack([dg_x,dg_y,dg_z])
dg_p = [FDEM.Src.RawVec_e([],_,dg/mesh.area) for _ in freqs]
# ------------ Problem and Survey ---------------
survey = FDEM.Survey(sg_p + dg_p)
mapping = [('sigma', Maps.IdentityMap(mesh))]
problem = FDEM.Problem3D_h(mesh, mapping=mapping)
problem.pair(survey)
# ------------- Solve ---------------------------
t0 = time.time()
fieldsCasing = problem.fields(sigCasing)
print 'Time to solve 2 sources', time.time() - t0
# Plot current
# current density
jn0 = fieldsCasing[dg_p,'j']
jn1 = fieldsCasing[sg_p,'j']
# current
in0 = [mesh.area*fieldsCasing[dg_p,'j'][:,i] for i in range(len(freqs))]
in1 = [mesh.area*fieldsCasing[sg_p,'j'][:,i] for i in range(len(freqs))]
in0 = np.vstack(in0).T
in1 = np.vstack(in1).T
# integrate to get z-current inside casing
inds_inx = (mesh.gridFz[:,0] >= casing_a) & (mesh.gridFz[:,0] <= casing_b)
inds_inz = (mesh.gridFz[:,2] >= dsz ) & (mesh.gridFz[:,2] <= 0)
inds_fz = inds_inx & inds_inz
indsx = [False]*mesh.nFx
inds = list(indsx) + list(inds_fz)
in0_in = in0[np.r_[inds]]
in1_in = in1[np.r_[inds]]
z_in = mesh.gridFz[inds_fz,2]
in0_in = in0_in.reshape([in0_in.shape[0]/3,3])
in1_in = in1_in.reshape([in1_in.shape[0]/3,3])
z_in = z_in.reshape([z_in.shape[0]/3,3])
I0 = in0_in.sum(1).real
I1 = in1_in.sum(1).real
z_in = z_in[:,0]
if plotIt is True:
fig, ax = plt.subplots(1,2,figsize=(12,4))
ax[0].plot(z_in,np.absolute(I0), z_in,np.absolute(I1))
ax[0].legend(['top casing', 'bottom casing'],loc='best')
ax[0].set_title('Magnitude of Vertical Current in Casing')
ax[1].semilogy(z_in,np.absolute(I0), z_in,np.absolute(I1))
ax[1].legend(['top casing', 'bottom casing'],loc='best')
ax[1].set_title('Magnitude of Vertical Current in Casing')
ax[1].set_ylim([1e-2, 1.])
plt.show()
if __name__ == '__main__':
run()
+132
View File
@@ -0,0 +1,132 @@
from SimPEG import *
def run(N=200, plotIt=True):
"""
Inversion: Linear Problem
=========================
Here we go over the basics of creating a linear problem and inversion.
"""
np.random.seed(1)
std_noise = 1e-2
mesh = Mesh.TensorMesh([N])
m0 = np.ones(mesh.nC) * 1e-4
nk = 10
jk = np.linspace(1.,nk,nk)
p = -2.
q = 1.
g = lambda k: np.exp(p*jk[k]*mesh.vectorCCx)*np.cos(np.pi*q*jk[k]*mesh.vectorCCx)
G = np.empty((nk, mesh.nC))
for i in range(nk):
G[i,:] = g(i)
mtrue = np.zeros(mesh.nC)
mtrue[mesh.vectorCCx > 0.3] = 1.
mtrue[mesh.vectorCCx > 0.45] = -0.5
mtrue[mesh.vectorCCx > 0.6] = 0
prob = Problem.LinearProblem(mesh, G)
survey = Survey.LinearSurvey()
survey.pair(prob)
survey.dobs = prob.fields(mtrue) + std_noise * np.random.randn(nk)
#survey.makeSyntheticData(mtrue, std=std_noise)
wd = np.ones(nk) * std_noise
#print survey.std[0]
#M = prob.mesh
# Distance weighting
wr = np.sum(prob.G**2.,axis=0)**0.5
wr = ( wr/np.max(wr) )
reg = Regularization.Simple(mesh)
reg.wght = wr
dmis = DataMisfit.l2_DataMisfit(survey)
dmis.Wd = 1./wd
opt = Optimization.ProjectedGNCG(maxIter=30,lower=-2.,upper=2., maxIterCG= 20, tolCG = 1e-4)
invProb = InvProblem.BaseInvProblem(dmis, reg, opt)
invProb.curModel = m0
beta = Directives.BetaSchedule(coolingFactor=2, coolingRate=1)
target = Directives.TargetMisfit()
betaest = Directives.BetaEstimate_ByEig()
inv = Inversion.BaseInversion(invProb, directiveList=[beta, betaest, target])
mrec = inv.run(m0)
ml2 = mrec
print "Final misfit:" + str(invProb.dmisfit.eval(mrec))
# Switch regularization to sparse
phim = invProb.phi_m_last
phid = invProb.phi_d
reg = Regularization.Sparse(mesh)
#==============================================================================
# fig, axes = plt.subplots(1,2,figsize=(12*1.2,4*1.2))
# dmdx = reg.mesh.cellDiffxStencil * mrec
# plt.plot(np.sort(dmdx))
#==============================================================================
#reg.recModel = mrec
reg.wght = np.ones(mesh.nC)
reg.mref = np.zeros(mesh.nC)
reg.eps_p = 5e-2
reg.eps_q = 1e-2
reg.norms = [0., 0., 2., 2.]
reg.wght = wr
opt = Optimization.ProjectedGNCG(maxIter=10 ,lower=-2.,upper=2., maxIterLS = 20, maxIterCG= 20, tolCG = 1e-3)
invProb = InvProblem.BaseInvProblem(dmis, reg, opt, beta = invProb.beta*2.)
beta = Directives.BetaSchedule(coolingFactor=1, coolingRate=1)
#betaest = Directives.BetaEstimate_ByEig()
target = Directives.TargetMisfit()
IRLS =Directives.Update_IRLS( phi_m_last = phim, phi_d_last = phid )
inv = Inversion.BaseInversion(invProb, directiveList=[beta,IRLS])
m0 = mrec
# Run inversion
mrec = inv.run(m0)
print "Final misfit:" + str(invProb.dmisfit.eval(mrec))
if plotIt:
import matplotlib.pyplot as plt
fig, axes = plt.subplots(1,2,figsize=(12*1.2,4*1.2))
for i in range(prob.G.shape[0]):
axes[0].plot(prob.G[i,:])
axes[0].set_title('Columns of matrix G')
axes[1].plot(mesh.vectorCCx, mtrue, 'b-')
axes[1].plot(mesh.vectorCCx, ml2, 'r-')
#axes[1].legend(('True Model', 'Recovered Model'))
axes[1].set_ylim(-1.0,1.25)
axes[1].plot(mesh.vectorCCx, mrec, 'k-',lw = 2)
axes[1].legend(('True Model', 'Smooth l2-l2',
'Sparse lp:' + str(reg.norms[0]) + ', lqx:' + str(reg.norms[1]) ), fontsize = 12)
plt.show()
return prob, survey, mesh, mrec
if __name__ == '__main__':
run()
+2 -24
View File
@@ -10,28 +10,6 @@ def run(N=100, plotIt=True):
"""
class LinearSurvey(Survey.BaseSurvey):
def eval(self, u):
return u
class LinearProblem(Problem.BaseProblem):
surveyPair = LinearSurvey
def __init__(self, mesh, G, **kwargs):
Problem.BaseProblem.__init__(self, mesh, **kwargs)
self.G = G
def fields(self, m, u=None):
return self.G.dot(m)
def Jvec(self, m, v, u=None):
return self.G.dot(v)
def Jtvec(self, m, v, u=None):
return self.G.T.dot(v)
np.random.seed(1)
mesh = Mesh.TensorMesh([N])
@@ -53,8 +31,8 @@ def run(N=100, plotIt=True):
mtrue[mesh.vectorCCx > 0.45] = -0.5
mtrue[mesh.vectorCCx > 0.6] = 0
prob = LinearProblem(mesh, G)
survey = LinearSurvey()
prob = Problem.LinearProblem(mesh, G)
survey = Survey.LinearSurvey()
survey.pair(prob)
survey.makeSyntheticData(mtrue, std=0.01)
+1 -1
View File
@@ -100,7 +100,7 @@ def run(plotIt=True):
# Regularization - with a regularization mesh
regMesh = simpeg.Mesh.TensorMesh([m1d.hx[problem.mapping.sigmaMap.maps[-1].indActive]],m1d.x0)
reg = simpeg.Regularization.Tikhonov(regMesh)
reg.smoothModel = True
reg.mrefInSmooth = True
reg.alpha_s = 1e-7
reg.alpha_x = 1.
# Inversion problem
+5 -1
View File
@@ -1,11 +1,15 @@
# Run this file to add imports.
##### AUTOIMPORTS #####
import DC_Analytic_Dipole
import DC_Forward_PseudoSection
import EM_FDEM_1D_Inversion
import EM_FDEM_Analytic_MagDipoleWholespace
import EM_Schenkel_Morrison_Casing
import EM_TDEM_1D_Inversion
import FLOW_Richards_1D_Celia1990
import Forward_BasicDirectCurrent
import Inversion_IRLS
import Inversion_Linear
import Mesh_Basic_PlotImage
import Mesh_Basic_Types
@@ -17,7 +21,7 @@ import Mesh_Tensor_Creation
import MT_1D_ForwardAndInversion
import MT_3D_Foward
__examples__ = ["EM_FDEM_1D_Inversion", "EM_FDEM_Analytic_MagDipoleWholespace", "EM_TDEM_1D_Inversion", "FLOW_Richards_1D_Celia1990", "Forward_BasicDirectCurrent", "Inversion_Linear", "Mesh_Basic_PlotImage", "Mesh_Basic_Types", "Mesh_Operators_CahnHilliard", "Mesh_QuadTree_Creation", "Mesh_QuadTree_FaceDiv", "Mesh_QuadTree_HangingNodes", "Mesh_Tensor_Creation", "MT_1D_ForwardAndInversion", "MT_3D_Foward"]
__examples__ = ["DC_Analytic_Dipole", "DC_Forward_PseudoSection", "EM_FDEM_1D_Inversion", "EM_FDEM_Analytic_MagDipoleWholespace", "EM_Schenkel_Morrison_Casing", "EM_TDEM_1D_Inversion", "FLOW_Richards_1D_Celia1990", "Forward_BasicDirectCurrent", "Inversion_IRLS", "Inversion_Linear", "Mesh_Basic_PlotImage", "Mesh_Basic_Types", "Mesh_Operators_CahnHilliard", "Mesh_QuadTree_Creation", "Mesh_QuadTree_FaceDiv", "Mesh_QuadTree_HangingNodes", "Mesh_Tensor_Creation", "MT_1D_ForwardAndInversion", "MT_3D_Foward"]
##### AUTOIMPORTS #####
+29 -29
View File
@@ -45,19 +45,19 @@ class RichardsSurvey(Survey.BaseSurvey):
@Utils.count
@Utils.requires('prob')
def dpred(self, m, u=None):
def dpred(self, m, f=None):
"""
Create the projected data from a model.
The field, u, (if provided) will be used for the predicted data
The field, f, (if provided) will be used for the predicted data
instead of recalculating the fields (which may be expensive!).
.. math::
d_\\text{pred} = P(u(m), m)
d_\\text{pred} = P(f(m), m)
Where P is a projection of the fields onto the data space.
"""
if u is None: u = self.prob.fields(m)
return Utils.mkvc(self.eval(u, m))
if f is None: f = self.prob.fields(m)
return Utils.mkvc(self.eval(f, m))
@Utils.requires('prob')
def eval(self, U, m):
@@ -233,16 +233,16 @@ class RichardsProblem(Problem.BaseTimeProblem):
return r, J
@Utils.timeIt
def Jfull(self, m, u=None):
if u is None:
u = self.fields(m)
def Jfull(self, m, f=None):
if f is None:
f = self.fields(m)
nn = len(u)-1
nn = len(f)-1
Asubs, Adiags, Bs = range(nn), range(nn), range(nn)
for ii in range(nn):
dt = self.timeSteps[ii]
bc = self.getBoundaryConditions(ii, u[ii])
Asubs[ii], Adiags[ii], Bs[ii] = self.diagsJacobian(m, u[ii], u[ii+1], dt, bc)
bc = self.getBoundaryConditions(ii, f[ii])
Asubs[ii], Adiags[ii], Bs[ii] = self.diagsJacobian(m, f[ii], f[ii+1], dt, bc)
Ad = sp.block_diag(Adiags)
zRight = Utils.spzeros((len(Asubs)-1)*Asubs[0].shape[0],Adiags[0].shape[1])
zTop = Utils.spzeros(Adiags[0].shape[0], len(Adiags)*Adiags[0].shape[1])
@@ -251,7 +251,7 @@ class RichardsProblem(Problem.BaseTimeProblem):
B = np.array(sp.vstack(Bs).todense())
Ainv = self.Solver(A, **self.solverOpts)
P = self.survey.evalDeriv(u, m)
P = self.survey.evalDeriv(f, m)
AinvB = Ainv * B
z = np.zeros((self.mesh.nC, B.shape[1]))
zAinvB = np.vstack((z, AinvB))
@@ -259,41 +259,41 @@ class RichardsProblem(Problem.BaseTimeProblem):
return J
@Utils.timeIt
def Jvec(self, m, v, u=None):
if u is None:
u = self.fields(m)
def Jvec(self, m, v, f=None):
if f is None:
f = self.fields(m)
JvC = range(len(u)-1) # Cell to hold each row of the long vector.
JvC = range(len(f)-1) # Cell to hold each row of the long vector.
# This is done via forward substitution.
bc = self.getBoundaryConditions(0, u[0])
temp, Adiag, B = self.diagsJacobian(m, u[0], u[1], self.timeSteps[0], bc)
bc = self.getBoundaryConditions(0, f[0])
temp, Adiag, B = self.diagsJacobian(m, f[0], f[1], self.timeSteps[0], bc)
Adiaginv = self.Solver(Adiag, **self.solverOpts)
JvC[0] = Adiaginv * (B*v)
for ii in range(1,len(u)-1):
bc = self.getBoundaryConditions(ii, u[ii])
Asub, Adiag, B = self.diagsJacobian(m, u[ii], u[ii+1], self.timeSteps[ii], bc)
for ii in range(1,len(f)-1):
bc = self.getBoundaryConditions(ii, f[ii])
Asub, Adiag, B = self.diagsJacobian(m, f[ii], f[ii+1], self.timeSteps[ii], bc)
Adiaginv = self.Solver(Adiag, **self.solverOpts)
JvC[ii] = Adiaginv * (B*v - Asub*JvC[ii-1])
P = self.survey.evalDeriv(u, m)
P = self.survey.evalDeriv(f, m)
return P * np.concatenate([np.zeros(self.mesh.nC)] + JvC)
@Utils.timeIt
def Jtvec(self, m, v, u=None):
if u is None:
u = self.field(m)
def Jtvec(self, m, v, f=None):
if f is None:
f = self.field(m)
P = self.survey.evalDeriv(u, m)
P = self.survey.evalDeriv(f, m)
PTv = P.T*v
# This is done via backward substitution.
minus = 0
BJtv = 0
for ii in range(len(u)-1,0,-1):
bc = self.getBoundaryConditions(ii-1, u[ii-1])
Asub, Adiag, B = self.diagsJacobian(m, u[ii-1], u[ii], self.timeSteps[ii-1], bc)
for ii in range(len(f)-1,0,-1):
bc = self.getBoundaryConditions(ii-1, f[ii-1])
Asub, Adiag, B = self.diagsJacobian(m, f[ii-1], f[ii], self.timeSteps[ii-1], bc)
#select the correct part of v
vpart = range((ii)*Adiag.shape[0], (ii+1)*Adiag.shape[0])
AdiaginvT = self.Solver(Adiag.T, **self.solverOpts)
+13 -13
View File
@@ -82,23 +82,23 @@ class BaseInvProblem(object):
self._warmstart = value
def getFields(self, m, store=False, deleteWarmstart=True):
u = None
f = None
for mtest, u_ofmtest in self.warmstart:
if m is mtest:
u = u_ofmtest
f = u_ofmtest
if self.debug: print 'InvProb is Warm Starting!'
break
if u is None:
u = self.prob.fields(m)
if f is None:
f = self.prob.fields(m)
if deleteWarmstart:
self.warmstart = []
if store:
self.warmstart += [(m,u)]
self.warmstart += [(m,f)]
return u
return f
@Utils.timeIt
def evalFunction(self, m, return_g=True, return_H=True):
@@ -109,21 +109,21 @@ class BaseInvProblem(object):
gc.collect()
# Store fields if doing a line-search
u = self.getFields(m, store=(return_g==False and return_H==False))
f = self.getFields(m, store=(return_g==False and return_H==False))
phi_d = self.dmisfit.eval(m, u=u)
phi_d = self.dmisfit.eval(m, f=f)
phi_m = self.reg.eval(m)
self.dpred = self.survey.dpred(m, u=u) # This is a cheap matrix vector calculation.
self.dpred = self.survey.dpred(m, f=f) # This is a cheap matrix vector calculation.
self.phi_d, self.phi_d_last = phi_d, self.phi_d
self.phi_m, self.phi_m_last = phi_m, self.phi_m
f = phi_d + self.beta * phi_m
phi = phi_d + self.beta * phi_m
out = (f,)
out = (phi,)
if return_g:
phi_dDeriv = self.dmisfit.evalDeriv(m, u=u)
phi_dDeriv = self.dmisfit.evalDeriv(m, f=f)
phi_mDeriv = self.reg.evalDeriv(m)
g = phi_dDeriv + self.beta * phi_mDeriv
@@ -131,7 +131,7 @@ class BaseInvProblem(object):
if return_H:
def H_fun(v):
phi_d2Deriv = self.dmisfit.eval2Deriv(m, v, u=u)
phi_d2Deriv = self.dmisfit.eval2Deriv(m, v, f=f)
phi_m2Deriv = self.reg.eval2Deriv(m, v=v)
return phi_d2Deriv + self.beta * phi_m2Deriv
+3 -1
View File
@@ -33,7 +33,9 @@ class BaseInversion(object):
self._directiveList = value
self._directiveList.inversion = self
def __init__(self, invProb, directiveList=[], **kwargs):
def __init__(self, invProb, directiveList=None, **kwargs):
if directiveList is None:
directiveList = []
self.directiveList = directiveList
Utils.setKwargs(self, **kwargs)
+13 -13
View File
@@ -27,7 +27,7 @@ class BaseMTProblem(BaseFDEMProblem):
# Might need to add more stuff here.
## NEED to clean up the Jvec and Jtvec to use Zero and Identities for None components.
def Jvec(self, m, v, u=None):
def Jvec(self, m, v, f=None):
"""
Function to calculate the data sensitivities dD/dm times a vector.
@@ -39,8 +39,8 @@ class BaseMTProblem(BaseFDEMProblem):
"""
# Calculate the fields
if u is None:
u = self.fields(m)
if f is None:
f= self.fields(m)
# Set current model
self.curModel = m
# Initiate the Jv object
@@ -56,9 +56,9 @@ class BaseMTProblem(BaseFDEMProblem):
# We need fDeriv_m = df/du*du/dm + df/dm
# Construct du/dm, it requires a solve
# NOTE: need to account for the 2 polarizations in the derivatives.
u_src = u[src,:]
f_src = f[src,:]
# dA_dm and dRHS_dm should be of size nE,2, so that we can multiply by dA_duI. The 2 columns are each of the polarizations.
dA_dm = self.getADeriv_m(freq, u_src, v) # Size: nE,2 (u_px,u_py) in the columns.
dA_dm = self.getADeriv_m(freq, f_src, v) # Size: nE,2 (u_px,u_py) in the columns.
dRHS_dm = self.getRHSDeriv_m(freq, v) # Size: nE,2 (u_px,u_py) in the columns.
if dRHS_dm is None:
du_dm = dA_duI * ( -dA_dm )
@@ -68,13 +68,13 @@ class BaseMTProblem(BaseFDEMProblem):
for rx in src.rxList:
# Get the projection derivative
# v should be of size 2*nE (for 2 polarizations)
PDeriv_u = lambda t: rx.evalDeriv(src, self.mesh, u, t) # wrt u, we don't have have PDeriv wrt m
PDeriv_u = lambda t: rx.evalDeriv(src, self.mesh, f, t) # wrt u, we don't have have PDeriv wrt m
Jv[src, rx] = PDeriv_u(mkvc(du_dm))
dA_duI.clean()
# Return the vectorized sensitivities
return mkvc(Jv)
def Jtvec(self, m, v, u=None):
def Jtvec(self, m, v, f=None):
"""
Function to calculate the transpose of the data sensitivities (dD/dm)^T times a vector.
@@ -85,8 +85,8 @@ class BaseMTProblem(BaseFDEMProblem):
:return: Data sensitivities wrt m
"""
if u is None:
u = self.fields(m)
if f is None:
f = self.fields(m)
self.curModel = m
@@ -103,15 +103,15 @@ class BaseMTProblem(BaseFDEMProblem):
for src in self.survey.getSrcByFreq(freq):
ftype = self._fieldType + 'Solution'
u_src = u[src, :]
f_src = f[src, :]
for rx in src.rxList:
# Get the adjoint evalDeriv
# PTv needs to be nE,
PTv = rx.evalDeriv(src, self.mesh, u, mkvc(v[src, rx],2), adjoint=True) # wrt u, need possibility wrt m
PTv = rx.evalDeriv(src, self.mesh, f, mkvc(v[src, rx],2), adjoint=True) # wrt u, need possibility wrt m
# Get the
dA_duIT = ATinv * PTv
dA_dmT = self.getADeriv_m(freq, u_src, mkvc(dA_duIT), adjoint=True)
dA_dmT = self.getADeriv_m(freq, f_src, mkvc(dA_duIT), adjoint=True)
dRHS_dmT = self.getRHSDeriv_m(freq, mkvc(dA_duIT), adjoint=True)
# Make du_dmT
if dRHS_dmT is None:
@@ -129,4 +129,4 @@ class BaseMTProblem(BaseFDEMProblem):
raise Exception('Must be real or imag')
# Clean the factorization, clear memory.
ATinv.clean()
return Jtv
return Jtv
+3 -3
View File
@@ -427,15 +427,15 @@ class Survey(SimPEGsurvey.BaseSurvey):
assert freq in self._freqDict, "The requested frequency is not in this survey."
return self._freqDict[freq]
def eval(self, u):
def eval(self, f):
data = Data(self)
for src in self.srcList:
sys.stdout.flush()
for rx in src.rxList:
data[src, rx] = rx.eval(src, self.mesh, u)
data[src, rx] = rx.eval(src, self.mesh, f)
return data
def evalDeriv(self, u):
def evalDeriv(self, f):
raise Exception('Use Transmitters to project fields deriv.')
#################
+12 -7
View File
@@ -7,17 +7,16 @@ from SimPEG.MT.Utils.dataUtils import rec2ndarr
# Import modules
import numpy as np
import os, sys, re
try:
import osr
except ImportError as e:
print 'Could not import osr, missing the gdal package'
pass
class EDIimporter:
"""
A class to import EDIfiles.
"""
# Define data converters
_impUnitEDI2SI = 4*np.pi*1e-4 # Convert Z[mV/km/nT] (as in EDI)to Z[V/A] SI unit
_impUnitSI2EDI = 1./_impUnitEDI2SI # ConvertZ[V/A] SI unit to Z[mV/km/nT] (as in EDI)
@@ -26,8 +25,8 @@ class EDIimporter:
comps = None
# Hidden properties
_outEPSG = None
_2out = None
_outEPSG = None # Project info
_2out = None # The projection operator
def __init__(self, EDIfilesList, compList=None, outEPSG=None):
@@ -113,6 +112,12 @@ class EDIimporter:
# nOutData=length(obj.data);
# obj.data(nOutData+1:nOutData+length(TEMP.data),:) = TEMP.data;
def _transfromPoints(self,longD,latD):
# Import the coordinate projections
try:
import osr
except ImportError as e:
print 'Could not import osr, missing the gdal package\nCan not project coordinates'
raise e
# Coordinates convertor
if self._2out is None:
src = osr.SpatialReference()
+26 -11
View File
@@ -759,15 +759,29 @@ class PolyMap(IdentityMap):
m = [\sigma_1, \sigma_2, c]
Can take in an actInd vector to account for topography.
"""
def __init__(self, mesh, order, logSigma=True, normal='X'):
def __init__(self, mesh, order, logSigma=True, normal='X', actInd = None):
IdentityMap.__init__(self, mesh)
self.logSigma = logSigma
self.order = order
self.normal = normal
self.actInd = actInd
if getattr(self, 'actInd', None) is None:
self.actInd = range(self.mesh.nC)
self.nC = self.mesh.nC
else:
self.nC = len(self.actInd)
slope = 1e4
@property
def shape(self):
return (self.nC, self.nP)
@property
def nP(self):
if np.isscalar(self.order):
@@ -785,8 +799,8 @@ class PolyMap(IdentityMap):
sig1, sig2 = np.exp(sig1), np.exp(sig2)
#2D
if self.mesh.dim == 2:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
if self.normal =='X':
f = polynomial.polyval(Y, c) - X
elif self.normal =='Y':
@@ -795,9 +809,9 @@ class PolyMap(IdentityMap):
raise(Exception("Input for normal = X or Y or Z"))
#3D
elif self.mesh.dim == 3:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
Z = self.mesh.gridCC[:,2]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
Z = self.mesh.gridCC[self.actInd,2]
if self.normal =='X':
f = polynomial.polyval2d(Y, Z, c.reshape((self.order[0]+1,self.order[1]+1))) - X
elif self.normal =='Y':
@@ -806,6 +820,7 @@ class PolyMap(IdentityMap):
f = polynomial.polyval2d(X, Y, c.reshape((self.order[0]+1,self.order[1]+1))) - Z
else:
raise(Exception("Input for normal = X or Y or Z"))
else:
raise(Exception("Only supports 2D"))
@@ -819,8 +834,8 @@ class PolyMap(IdentityMap):
sig1, sig2 = np.exp(sig1), np.exp(sig2)
#2D
if self.mesh.dim == 2:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
if self.normal =='X':
f = polynomial.polyval(Y, c) - X
@@ -832,9 +847,9 @@ class PolyMap(IdentityMap):
raise(Exception("Input for normal = X or Y or Z"))
#3D
elif self.mesh.dim == 3:
X = self.mesh.gridCC[:,0]
Y = self.mesh.gridCC[:,1]
Z = self.mesh.gridCC[:,2]
X = self.mesh.gridCC[self.actInd,0]
Y = self.mesh.gridCC[self.actInd,1]
Z = self.mesh.gridCC[self.actInd,2]
if self.normal =='X':
f = polynomial.polyval2d(Y, Z, c.reshape((self.order[0]+1,self.order[1]+1))) - X
+12 -9
View File
@@ -330,7 +330,7 @@ class CylMesh(BaseTensorMesh, BaseRectangularMesh, InnerProducts, CylView):
raise NotImplementedError('wrapping in the averaging is not yet implemented')
return self._aveF2CCV
def getInterpolationMatCartMesh(self, Mrect, locType='CC'):
def getInterpolationMatCartMesh(self, Mrect, locType='CC', locTypeTo=None):
"""
Takes a cartesian mesh and returns a projection to translate onto the cartesian grid.
"""
@@ -338,19 +338,22 @@ class CylMesh(BaseTensorMesh, BaseRectangularMesh, InnerProducts, CylView):
assert self.isSymmetric, "Currently we have not taken into account other projections for more complicated CylMeshes"
if locTypeTo is None:
locTypeTo = locType
if locType == 'F':
# do this three times for each component
X = self.getInterpolationMatCartMesh(Mrect, locType='Fx')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Fy')
Z = self.getInterpolationMatCartMesh(Mrect, locType='Fz')
X = self.getInterpolationMatCartMesh(Mrect, locType='Fx', locTypeTo=locTypeTo+'x')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Fy', locTypeTo=locTypeTo+'y')
Z = self.getInterpolationMatCartMesh(Mrect, locType='Fz', locTypeTo=locTypeTo+'z')
return sp.vstack((X,Y,Z))
if locType == 'E':
X = self.getInterpolationMatCartMesh(Mrect, locType='Ex')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Ey')
Z = spzeros(Mrect.nEz, self.nE)
X = self.getInterpolationMatCartMesh(Mrect, locType='Ex', locTypeTo=locTypeTo+'x')
Y = self.getInterpolationMatCartMesh(Mrect, locType='Ey', locTypeTo=locTypeTo+'y')
Z = spzeros(getattr(Mrect, 'n' + locTypeTo + 'z'), self.nE)
return sp.vstack((X,Y,Z))
grid = getattr(Mrect, 'grid' + locType)
grid = getattr(Mrect, 'grid' + locTypeTo)
# This is unit circle stuff, 0 to 2*pi, starting at x-axis, rotating counter clockwise in an x-y slice
theta = - np.arctan2(grid[:,0] - self.cartesianOrigin[0], grid[:,1] - self.cartesianOrigin[1]) + np.pi/2
theta[theta < 0] += np.pi*2.0
@@ -366,7 +369,7 @@ class CylMesh(BaseTensorMesh, BaseRectangularMesh, InnerProducts, CylView):
'Ex': Mrect.tangents[:Mrect.nEx,:],
'Ey': Mrect.tangents[Mrect.nEx:(Mrect.nEx+Mrect.nEy),:],
'Ez': Mrect.tangents[-Mrect.nEz:,:],
}[locType]
}[locTypeTo]
if 'F' in locType:
normals = np.c_[np.cos(theta), np.sin(theta), np.zeros(theta.size)]
proj = ( normals * dotMe ).sum(axis=1)
+49 -31
View File
@@ -307,24 +307,28 @@ class DiffOperators(object):
return BC
_cellGradBC_list = 'neumann'
def _cellGradStencil(self):
BC = self.setCellGradBC(self._cellGradBC_list)
n = self.vnC
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")
return G
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_list)
n = self.vnC
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")
G = self._cellGradStencil()
# Compute areas of cell faces & volumes
S = self.area
V = self.aveCC2F*self.vol # Average volume between adjacent cells
@@ -361,19 +365,24 @@ class DiffOperators(object):
_cellGradBC = None
cellGradBC = property(**cellGradBC())
def _cellGradxStencil(self):
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 1):
G1 = ddxCellGrad(n[0], BC)
elif(self.dim == 2):
G1 = sp.kron(speye(n[1]), ddxCellGrad(n[0], BC))
elif(self.dim == 3):
G1 = kron3(speye(n[2]), speye(n[1]), ddxCellGrad(n[0], BC))
return G1
def cellGradx():
doc = "Cell centered Gradient in the x dimension. Has neumann boundary conditions."
def fget(self):
if getattr(self, '_cellGradx', None) is None:
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 1):
G1 = ddxCellGrad(n[0], BC)
elif(self.dim == 2):
G1 = sp.kron(speye(n[1]), ddxCellGrad(n[0], BC))
elif(self.dim == 3):
G1 = kron3(speye(n[2]), speye(n[1]), ddxCellGrad(n[0], BC))
G1 = self._cellGradxStencil()
# Compute areas of cell faces & volumes
V = self.aveCC2F*self.vol
L = self.r(self.area/V, 'F','Fx', 'V')
@@ -382,17 +391,22 @@ class DiffOperators(object):
return locals()
cellGradx = property(**cellGradx())
def _cellGradyStencil(self):
if self.dim < 2: return None
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 2):
G2 = sp.kron(ddxCellGrad(n[1], BC), speye(n[0]))
elif(self.dim == 3):
G2 = kron3(speye(n[2]), ddxCellGrad(n[1], BC), speye(n[0]))
return G2
def cellGrady():
doc = "Cell centered Gradient in the x dimension. Has neumann boundary conditions."
def fget(self):
if self.dim < 2: return None
if getattr(self, '_cellGrady', None) is None:
BC = ['neumann', 'neumann']
n = self.vnC
if(self.dim == 2):
G2 = sp.kron(ddxCellGrad(n[1], BC), speye(n[0]))
elif(self.dim == 3):
G2 = kron3(speye(n[2]), ddxCellGrad(n[1], BC), speye(n[0]))
G2 = self._cellGradyStencil()
# Compute areas of cell faces & volumes
V = self.aveCC2F*self.vol
L = self.r(self.area/V, 'F','Fy', 'V')
@@ -401,14 +415,19 @@ class DiffOperators(object):
return locals()
cellGrady = property(**cellGrady())
def _cellGradzStencil(self):
if self.dim < 3: return None
BC = ['neumann', 'neumann']
n = self.vnC
G3 = kron3(ddxCellGrad(n[2], BC), speye(n[1]), speye(n[0]))
return G3
def cellGradz():
doc = "Cell centered Gradient in the x dimension. Has neumann boundary conditions."
def fget(self):
if self.dim < 3: return None
if getattr(self, '_cellGradz', None) is None:
BC = ['neumann', 'neumann']
n = self.vnC
G3 = kron3(ddxCellGrad(n[2], BC), speye(n[1]), speye(n[0]))
G3 = self._cellGradzStencil()
# Compute areas of cell faces & volumes
V = self.aveCC2F*self.vol
L = self.r(self.area/V, 'F','Fz', 'V')
@@ -746,4 +765,3 @@ class DiffOperators(object):
kron3(av(n[2]), speye(n[1]+1), av(n[0])),
kron3(speye(n[2]+1), av(n[1]), av(n[0]))), format="csr")
return self._aveN2F
+1 -2
View File
@@ -21,10 +21,9 @@ class TensorMeshIO(object):
if '*' in seg:
st = seg
sp = seg.split('*')
re = np.array(sp[0],dtype=int)*(' ' + sp[1])
re = int(sp[0])*(' ' + sp[1])
line = line.replace(st,re.strip())
return np.array(line.split(),dtype=float)
# Read the file as line strings, remove lines with comment = !
msh = np.genfromtxt(fileName,delimiter='\n',dtype=np.str,comments='!')
+13
View File
@@ -234,6 +234,9 @@ class BaseTensorMesh(BaseMesh):
'Fz' -> z-component of field defined on faces
'N' -> scalar field defined on nodes
'CC' -> scalar field defined on cell centers
'CCVx' -> x-component of vector field defined on cell centers
'CCVy' -> y-component of vector field defined on cell centers
'CCVz' -> z-component of vector field defined on cell centers
"""
if self._meshType == 'CYL' and self.isSymmetric and locType in ['Ex','Ez','Fy']:
raise Exception('Symmetric CylMesh does not support %s interpolation, as this variable does not exist.' % locType)
@@ -257,6 +260,16 @@ class BaseTensorMesh(BaseMesh):
Q = sp.hstack(components)
elif locType in ['CC', 'N']:
Q = Utils.interpmat(loc, *self.getTensor(locType))
elif locType in ['CCVx', 'CCVy', 'CCVz']:
Q = Utils.interpmat(loc, *self.getTensor('CC'))
Z = Utils.spzeros(loc.shape[0],self.nC)
if locType == 'CCVx':
Q = sp.hstack([Q,Z,Z])
elif locType == 'CCVy':
Q = sp.hstack([Z,Q,Z])
elif locType == 'CCVz':
Q = sp.hstack([Z,Z,Q])
else:
raise NotImplementedError('getInterpolationMat: locType=='+locType+' and mesh.dim=='+str(self.dim))
+9 -3
View File
@@ -2131,10 +2131,16 @@ class TreeMesh(BaseTensorMesh, InnerProducts, TreeMeshIO):
def plotSlice(self, v, vType='CC',
normal='Z', ind=None, grid=True, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k', 'alpha':0.5}):
pcolorOpts=None,
streamOpts=None,
gridOpts=None):
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k', 'alpha':0.5}
assert vType in ['CC','F','E']
assert self.dim == 3
+27 -9
View File
@@ -42,9 +42,9 @@ class TensorView(object):
def plotImage(self, v, vType='CC', grid=False, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k'},
pcolorOpts=None,
streamOpts=None,
gridOpts=None,
numbering=True, annotationColor='w'
):
"""
@@ -84,6 +84,12 @@ class TensorView(object):
M.plotImage(v, annotationColor='k', showIt=True)
"""
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k'}
if ax is None:
fig = plt.figure()
@@ -174,9 +180,9 @@ class TensorView(object):
def plotSlice(self, v, vType='CC',
normal='Z', ind=None, grid=False, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k', 'alpha':0.5}
pcolorOpts=None,
streamOpts=None,
gridOpts=None
):
"""
@@ -197,6 +203,12 @@ class TensorView(object):
M.plotSlice(M.cellGrad*b, 'F', view='vec', grid=True, showIt=True, pcolorOpts={'alpha':0.8})
"""
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k', 'alpha':0.5}
if type(vType) in [list, tuple]:
assert ax is None, "cannot specify an axis to plot on with this function."
fig, axs = plt.subplots(1,len(vType))
@@ -289,11 +301,17 @@ class TensorView(object):
def _plotImage2D(self, v, vType='CC', grid=False, view='real',
ax=None, clim=None, showIt=False,
pcolorOpts={},
streamOpts={'color':'k'},
gridOpts={'color':'k'}
pcolorOpts=None,
streamOpts=None,
gridOpts=None
):
if pcolorOpts is None:
pcolorOpts = {}
if streamOpts is None:
streamOpts = {'color':'k'}
if gridOpts is None:
gridOpts = {'color':'k'}
vTypeOptsCC = ['N','CC','Fx','Fy','Ex','Ey']
vTypeOptsV = ['CCv','F','E']
vTypeOpts = vTypeOptsCC + vTypeOptsV
+18
View File
@@ -888,6 +888,8 @@ class ProjectedGNCG(BFGS, Minimize, Remember):
maxIterCG = 5
tolCG = 1e-1
stepOffBoundsFact = 0.1 # perturbation of the inactive set off the bounds
lower = -np.inf
upper = np.inf
@@ -990,4 +992,20 @@ class ProjectedGNCG(BFGS, Minimize, Remember):
cgFlag = 1
# End CG Iterations
# Take a gradient step on the active cells if exist
if temp != self.xc.size:
rhs_a = (Active) * -self.g
dm_i = max( abs( delx ) )
dm_a = max( abs(rhs_a) )
# perturb inactive set off of bounds so that they are included in the step
delx = delx + self.stepOffBoundsFact * (rhs_a * dm_i / dm_a)
# Only keep gradients going in the right direction on the active set
indx = ((self.xc<=self.lower) & (delx < 0)) | ((self.xc>=self.upper) & (delx > 0))
delx[indx] = 0.
return delx
+29 -14
View File
@@ -88,28 +88,28 @@ class BaseProblem(object):
return self.survey is not None
@Utils.timeIt
def Jvec(self, m, v, u=None):
"""Jvec(m, v, u=None)
def Jvec(self, m, v, f=None):
"""Jvec(m, v, f=None)
Effect of J(m) on a vector v.
:param numpy.array m: model
:param numpy.array v: vector to multiply
:param numpy.array u: fields
:param Fields f: fields
:rtype: numpy.array
:return: Jv
"""
raise NotImplementedError('J is not yet implemented.')
@Utils.timeIt
def Jtvec(self, m, v, u=None):
"""Jtvec(m, v, u=None)
def Jtvec(self, m, v, f=None):
"""Jtvec(m, v, f=None)
Effect of transpose of J(m) on a vector v.
:param numpy.array m: model
:param numpy.array v: vector to multiply
:param numpy.array u: fields
:param Fields f: fields
:rtype: numpy.array
:return: JTv
"""
@@ -117,32 +117,32 @@ class BaseProblem(object):
@Utils.timeIt
def Jvec_approx(self, m, v, u=None):
"""Jvec_approx(m, v, u=None)
def Jvec_approx(self, m, v, f=None):
"""Jvec_approx(m, v, f=None)
Approximate effect of J(m) on a vector v
:param numpy.array m: model
:param numpy.array v: vector to multiply
:param numpy.array u: fields
:param Fields f: fields
:rtype: numpy.array
:return: approxJv
"""
return self.Jvec(m, v, u)
return self.Jvec(m, v, f)
@Utils.timeIt
def Jtvec_approx(self, m, v, u=None):
"""Jtvec_approx(m, v, u=None)
def Jtvec_approx(self, m, v, f=None):
"""Jtvec_approx(m, v, f=None)
Approximate effect of transpose of J(m) on a vector v.
:param numpy.array m: model
:param numpy.array v: vector to multiply
:param numpy.array u: fields
:param Fields f: fields
:rtype: numpy.array
:return: JTv
"""
return self.Jtvec(m, v, u)
return self.Jtvec(m, v, f)
def fields(self, m):
"""
@@ -213,5 +213,20 @@ class BaseTimeProblem(BaseProblem):
if hasattr(self, '_timeMesh'):
del self._timeMesh
class LinearProblem(BaseProblem):
surveyPair = Survey.LinearSurvey
def __init__(self, mesh, G, **kwargs):
BaseProblem.__init__(self, mesh, **kwargs)
self.G = G
def fields(self, m):
return self.G.dot(m)
def Jvec(self, m, v, f=None):
return self.G.dot(v)
def Jtvec(self, m, v, f=None):
return self.G.T.dot(v)
+557 -97
View File
@@ -1,5 +1,289 @@
import Utils, Maps, Mesh, numpy as np, scipy.sparse as sp
class RegularizationMesh(object):
"""
**Regularization Mesh**
This contains the operators used in the regularization. Note that these
are not necessarily true differential operators, but are constructed from
a SimPEG Mesh.
:param Mesh mesh: problem mesh
:param numpy.array indActive: bool array, size nC, that is True where we have active cells. Used to reduce the operators so we regularize only on active cells
"""
def __init__(self, mesh, indActive=None):
self.mesh = mesh
assert indActive is None or indActive.dtype == 'bool', 'indActive needs to be None or a bool'
self.indActive = indActive
@property
def vol(self):
"""
reduced volume vector
:rtype: numpy.array
:return: reduced cell volume
"""
if getattr(self, '_vol', None) is None:
self._vol = self._Pac.T * self.mesh.vol
return self._vol
@property
def nC(self):
"""
reduced number of cells
:rtype: int
:return: number of cells being regularized
"""
if getattr(self, '_nC', None) is None:
if self.indActive is None:
self._nC = self.mesh.nC
else:
self._nC = sum(self.indActive)
return self._nC
@property
def dim(self):
"""
dimension of regularization mesh (1D, 2D, 3D)
:rtype: int
:return: dimension
"""
if getattr(self, '_dim', None) is None:
self._dim = self.mesh.dim
return self._dim
@property
def _Pac(self):
"""
projection matrix that takes from the reduced space of active cells to full modelling space (ie. nC x nindActive)
:rtype: scipy.sparse.csr_matrix
:return: active cell projection matrix
"""
if getattr(self, '__Pac', None) is None:
if self.indActive is None:
self.__Pac = Utils.speye(self.mesh.nC)
else:
self.__Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
return self.__Pac
@property
def _Pafx(self):
"""
projection matrix that takes from the reduced space of active x-faces to full modelling space (ie. nFx x nindActive_Fx )
:rtype: scipy.sparse.csr_matrix
:return: active face-x projection matrix
"""
if getattr(self, '__Pafx', None) is None:
if self.indActive is None:
self.__Pafx = Utils.speye(self.mesh.nFx)
else:
indActive_Fx = (self.mesh.aveFx2CC.T * self.indActive) == 1
self.__Pafx = Utils.speye(self.mesh.nFx)[:,indActive_Fx]
return self.__Pafx
@property
def _Pafy(self):
"""
projection matrix that takes from the reduced space of active y-faces to full modelling space (ie. nFy x nindActive_Fy )
:rtype: scipy.sparse.csr_matrix
:return: active face-y projection matrix
"""
if getattr(self, '__Pafy', None) is None:
if self.indActive is None:
self.__Pafy = Utils.speye(self.mesh.nFy)
else:
indActive_Fy = (self.mesh.aveFy2CC.T * self.indActive) == 1
self.__Pafy = Utils.speye(self.mesh.nFy)[:,indActive_Fy]
return self.__Pafy
@property
def _Pafz(self):
"""
projection matrix that takes from the reduced space of active z-faces to full modelling space (ie. nFz x nindActive_Fz )
:rtype: scipy.sparse.csr_matrix
:return: active face-z projection matrix
"""
if getattr(self, '__Pafz', None) is None:
if self.indActive is None:
self.__Pafz = Utils.speye(self.mesh.nFz)
else:
indActive_Fz = (self.mesh.aveFz2CC.T * self.indActive) == 1
self.__Pafz = Utils.speye(self.mesh.nFz)[:,indActive_Fz]
return self.__Pafz
@property
def aveFx2CC(self):
"""
averaging from active cell centers to active x-faces
:rtype: scipy.sparse.csr_matrix
:return: averaging from active cell centers to active x-faces
"""
if getattr(self, '_aveFx2CC', None) is None:
self._aveFx2CC = self._Pac.T * self.mesh.aveFx2CC * self._Pafx
return self._aveFx2CC
@property
def aveCC2Fx(self):
"""
averaging from active x-faces to active cell centers
:rtype: scipy.sparse.csr_matrix
:return: averaging matrix from active x-faces to active cell centers
"""
if getattr(self, '_aveCC2Fx', None) is None:
self._aveCC2Fx = Utils.sdiag(1./(self.aveFx2CC.T).sum(1)) * self.aveFx2CC.T
return self._aveCC2Fx
@property
def aveFy2CC(self):
"""
averaging from active cell centers to active y-faces
:rtype: scipy.sparse.csr_matrix
:return: averaging from active cell centers to active y-faces
"""
if getattr(self, '_aveFy2CC', None) is None:
self._aveFy2CC = self._Pac.T * self.mesh.aveFy2CC * self._Pafy
return self._aveFy2CC
@property
def aveCC2Fy(self):
"""
averaging from active y-faces to active cell centers
:rtype: scipy.sparse.csr_matrix
:return: averaging matrix from active y-faces to active cell centers
"""
if getattr(self, '_aveCC2Fy', None) is None:
self._aveCC2Fy = Utils.sdiag(1./(self.aveFy2CC.T).sum(1)) * self.aveFy2CC.T
return self._aveCC2Fy
@property
def aveFz2CC(self):
"""
averaging from active cell centers to active z-faces
:rtype: scipy.sparse.csr_matrix
:return: averaging from active cell centers to active z-faces
"""
if getattr(self, '_aveFz2CC', None) is None:
self._aveFz2CC = self._Pac.T * self.mesh.aveFz2CC * self._Pafz
return self._aveFz2CC
@property
def aveCC2Fz(self):
"""
averaging from active z-faces to active cell centers
:rtype: scipy.sparse.csr_matrix
:return: averaging matrix from active z-faces to active cell centers
"""
if getattr(self, '_aveCC2Fz', None) is None:
self._aveCC2Fz = Utils.sdiag(1./(self.aveFz2CC.T).sum(1)) * self.aveFz2CC.T
return self._aveCC2Fz
@property
def cellDiffx(self):
"""
cell centered difference in the x-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the x-direction
"""
if getattr(self, '_cellDiffx', None) is None:
self._cellDiffx = self._Pafx.T * self.mesh.cellGradx * self._Pac
return self._cellDiffx
@property
def cellDiffy(self):
"""
cell centered difference in the y-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the y-direction
"""
if getattr(self, '_cellDiffy', None) is None:
self._cellDiffy = self._Pafy.T * self.mesh.cellGrady * self._Pac
return self._cellDiffy
@property
def cellDiffz(self):
"""
cell centered difference in the z-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the z-direction
"""
if getattr(self, '_cellDiffz', None) is None:
self._cellDiffz = self._Pafz.T * self.mesh.cellGradz * self._Pac
return self._cellDiffz
@property
def faceDiffx(self):
"""
x-face differences
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active faces in the x-direction
"""
if getattr(self, '_faceDiffx', None) is None:
self._faceDiffx = self._Pac.T * self.mesh.faceDivx * self._Pafx
return self._faceDiffx
@property
def faceDiffy(self):
"""
y-face differences
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active faces in the y-direction
"""
if getattr(self, '_faceDiffy', None) is None:
self._faceDiffy = self._Pac.T * self.mesh.faceDivy * self._Pafy
return self._faceDiffy
@property
def faceDiffz(self):
"""
z-face differences
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active faces in the z-direction
"""
if getattr(self, '_faceDiffz', None) is None:
self._faceDiffz = self._Pac.T * self.mesh.faceDivz * self._Pafz
return self._faceDiffz
@property
def cellDiffxStencil(self):
"""
cell centered difference stencil (no cell lengths include) in the x-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the x-direction
"""
if getattr(self, '_cellDiffxStencil', None) is None:
self._cellDiffxStencil = self._Pafx.T * self.mesh._cellGradxStencil() * self._Pac
return self._cellDiffxStencil
@property
def cellDiffyStencil(self):
"""
cell centered difference stencil (no cell lengths include) in the y-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the y-direction
"""
if self.dim < 2: return None
if getattr(self, '_cellDiffyStencil', None) is None:
self._cellDiffyStencil = self._Pafy.T * self.mesh._cellGradyStencil() * self._Pac
return self._cellDiffyStencil
@property
def cellDiffzStencil(self):
"""
cell centered difference stencil (no cell lengths include) in the y-direction
:rtype: scipy.sparse.csr_matrix
:return: differencing matrix for active cells in the y-direction
"""
if self.dim < 3: return None
if getattr(self, '_cellDiffzStencil', None) is None:
self._cellDiffzStencil = self._Pafz.T * self.mesh._cellGradzStencil() * self._Pac
return self._cellDiffzStencil
class BaseRegularization(object):
"""
**Base Regularization Class**
@@ -18,12 +302,19 @@ class BaseRegularization(object):
mapping = None #: A SimPEG.Map instance.
mesh = None #: A SimPEG.Mesh instance.
mref = None #: Reference model.
mref = None #: Reference model.
def __init__(self, mesh, mapping=None, indActive=None, **kwargs):
Utils.setKwargs(self, **kwargs)
self.mesh = mesh
assert isinstance(mesh, Mesh.BaseMesh), "mesh must be a SimPEG.Mesh object."
if indActive is not None and indActive.dtype != 'bool':
tmp = indActive
indActive = np.zeros(mesh.nC, dtype=bool)
indActive[tmp] = True
if indActive is not None and mapping is None:
mapping = Maps.IdentityMap(nP=indActive.nonzero()[0].size)
self.regmesh = RegularizationMesh(mesh,indActive)
self.mapping = mapping or self.mapPair(mesh)
self.mapping._assertMatchesPair(self.mapPair)
self.indActive = indActive
@@ -55,8 +346,7 @@ class BaseRegularization(object):
@property
def W(self):
"""Full regularization weighting matrix W."""
return sp.identity(self.mapping.nP)
return sp.identity(self.regmesh.nC)
@Utils.timeIt
def eval(self, m):
@@ -87,11 +377,12 @@ class BaseRegularization(object):
@Utils.timeIt
def eval2Deriv(self, m, v=None):
"""
Second derivative
:param numpy.array m: geophysical model
:param numpy.array v: vector to multiply
:rtype: scipy.sparse.csr_matrix or numpy.ndarray
:return: WtW or WtW*v
:param numpy.array m: geophysical model
:param numpy.array v: vector to multiply
:rtype: scipy.sparse.csr_matrix or numpy.ndarray
:return: WtW or WtW*v
The regularization is:
@@ -112,112 +403,94 @@ class BaseRegularization(object):
return mD.T * ( self.W.T * ( self.W * ( mD * v) ) )
class Tikhonov(BaseRegularization):
"""
L2 Tikhonov regularization with both smallness and smoothness (first order
derivative) contributions.
.. math::
\phi_m(\mathbf{m}) = \\alpha_s \| W_s (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
+ \\alpha_x \| W_x \\frac{\partial}{\partial x} (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
+ \\alpha_y \| W_y \\frac{\partial}{\partial y} (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
+ \\alpha_z \| W_z \\frac{\partial}{\partial z} (\mathbf{m} - \mathbf{m_{ref}} ) \|^2
Note if the key word argument `mrefInSmooth` is False, then mref is not
included in the smoothness contribution.
:param Mesh mesh: SimPEG mesh
:param Maps mapping: regularization mapping, takes the model from model space to the thing you want to regularize
:param numpy.ndarray indActive: active cell indices for reducing the size of differential operators in the definition of a regularization mesh
:param bool mrefInSmooth: (default = False) put mref in the smoothness component?
:param float alpha_s: (default 1e-6) smallness weight
:param float alpha_x: (default 1) smoothness weight for first derivative in the x-direction
:param float alpha_y: (default 1) smoothness weight for first derivative in the y-direction
:param float alpha_z: (default 1) smoothness weight for first derivative in the z-direction
:param float alpha_xx: (default 1) smoothness weight for second derivative in the x-direction
:param float alpha_yy: (default 1) smoothness weight for second derivative in the y-direction
:param float alpha_zz: (default 1) smoothness weight for second derivative in the z-direction
"""
smoothModel = True #: SMOOTH and SMOOTH_MOD_DIF options
alpha_s = Utils.dependentProperty('_alpha_s', 1e-6, ['_W', '_Ws'], "Smallness weight")
alpha_x = Utils.dependentProperty('_alpha_x', 1.0, ['_W', '_Wx'], "Weight for the first derivative in the x direction")
alpha_y = Utils.dependentProperty('_alpha_y', 1.0, ['_W', '_Wy'], "Weight for the first derivative in the y direction")
alpha_z = Utils.dependentProperty('_alpha_z', 1.0, ['_W', '_Wz'], "Weight for the first derivative in the z direction")
alpha_xx = Utils.dependentProperty('_alpha_xx', 0.0, ['_W', '_Wxx'], "Weight for the second derivative in the x direction")
alpha_yy = Utils.dependentProperty('_alpha_yy', 0.0, ['_W', '_Wyy'], "Weight for the second derivative in the y direction")
alpha_zz = Utils.dependentProperty('_alpha_zz', 0.0, ['_W', '_Wzz'], "Weight for the second derivative in the z direction")
mrefInSmooth = False # put mref in the smoothness contribution
alpha_s = Utils.dependentProperty('_alpha_s', 1e-6, ['_W', '_Wsmall'], "Smallness weight")
alpha_x = Utils.dependentProperty('_alpha_x', 1.0, ['_W', '_Wx'], "Weight for the first derivative in the x direction")
alpha_y = Utils.dependentProperty('_alpha_y', 1.0, ['_W', '_Wy'], "Weight for the first derivative in the y direction")
alpha_z = Utils.dependentProperty('_alpha_z', 1.0, ['_W', '_Wz'], "Weight for the first derivative in the z direction")
alpha_xx = Utils.dependentProperty('_alpha_xx', 0.0, ['_W', '_Wxx'], "Weight for the second derivative in the x direction")
alpha_yy = Utils.dependentProperty('_alpha_yy', 0.0, ['_W', '_Wyy'], "Weight for the second derivative in the y direction")
alpha_zz = Utils.dependentProperty('_alpha_zz', 0.0, ['_W', '_Wzz'], "Weight for the second derivative in the z direction")
def __init__(self, mesh, mapping=None, indActive = None, **kwargs):
BaseRegularization.__init__(self, mesh, mapping=mapping, **kwargs)
self.indActive = indActive
BaseRegularization.__init__(self, mesh, mapping=mapping, indActive=indActive, **kwargs)
@property
def Ws(self):
"""Regularization matrix Ws"""
if getattr(self,'_Ws', None) is None:
self._Ws = Utils.sdiag((self.mesh.vol*self.alpha_s)**0.5)
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Ws = Pac.T * self._Ws * Pac
return self._Ws
def Wsmall(self):
"""Regularization matrix Wsmall"""
if getattr(self,'_Wsmall', None) is None:
self._Wsmall = Utils.sdiag((self.regmesh.vol*self.alpha_s)**0.5)
return self._Wsmall
@property
def Wx(self):
"""Regularization matrix Wx"""
if getattr(self, '_Wx', None) is None:
Ave_x_vol = self.mesh.aveF2CC[:,:self.mesh.nFx].T*self.mesh.vol
self._Wx = Utils.sdiag((Ave_x_vol*self.alpha_x)**0.5)*self.mesh.cellGradx
if self.indActive is not None:
indActive_Fx = (self.mesh.aveFx2CC.T * self.indActive) == 1
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
Pafx = Utils.speye(self.mesh.nFx)[:,indActive_Fx]
self._Wx = Pafx.T*self._Wx*Pac
Ave_x_vol = self.regmesh.aveCC2Fx * self.regmesh.vol
self._Wx = Utils.sdiag((Ave_x_vol*self.alpha_x)**0.5)*self.regmesh.cellDiffx
return self._Wx
@property
def Wy(self):
"""Regularization matrix Wy"""
if getattr(self, '_Wy', None) is None:
Ave_y_vol = self.mesh.aveF2CC[:,self.mesh.nFx:np.sum(self.mesh.vnF[:2])].T*self.mesh.vol
self._Wy = Utils.sdiag((Ave_y_vol*self.alpha_y)**0.5)*self.mesh.cellGrady
if self.indActive is not None:
indActive_Fy = (self.mesh.aveFy2CC.T * self.indActive) == 1
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
Pafy = Utils.speye(self.mesh.nFy)[:,indActive_Fy]
self._Wy = Pafy.T*self._Wy*Pac
Ave_y_vol = self.regmesh.aveCC2Fy * self.regmesh.vol
self._Wy = Utils.sdiag((Ave_y_vol*self.alpha_y)**0.5)*self.regmesh.cellDiffy
return self._Wy
@property
def Wz(self):
"""Regularization matrix Wz"""
if getattr(self, '_Wz', None) is None:
Ave_z_vol = self.mesh.aveF2CC[:,np.sum(self.mesh.vnF[:2]):].T*self.mesh.vol
self._Wz = Utils.sdiag((Ave_z_vol*self.alpha_z)**0.5)*self.mesh.cellGradz
if self.indActive is not None:
indActive_Fz = (self.mesh.aveFz2CC.T * self.indActive) == 1
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
Pafz = Utils.speye(self.mesh.nFz)[:,indActive_Fz]
self._Wz = Pafz.T*self._Wz*Pac
Ave_z_vol = self.regmesh.aveCC2Fz * self.regmesh.vol
self._Wz = Utils.sdiag((Ave_z_vol*self.alpha_z)**0.5)*self.regmesh.cellDiffz
return self._Wz
@property
def Wxx(self):
"""Regularization matrix Wxx"""
if getattr(self, '_Wxx', None) is None:
self._Wxx = Utils.sdiag((self.mesh.vol*self.alpha_xx)**0.5)*self.mesh.faceDivx*self.mesh.cellGradx
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Wxx = Pac.T*self._Wxx*Pac
self._Wxx = Utils.sdiag((self.regmesh.vol*self.alpha_xx)**0.5)*self.regmesh.faceDiffx*self.regmesh.cellDiffx
return self._Wxx
@property
def Wyy(self):
"""Regularization matrix Wyy"""
if getattr(self, '_Wyy', None) is None:
self._Wyy = Utils.sdiag((self.mesh.vol*self.alpha_yy)**0.5)*self.mesh.faceDivy*self.mesh.cellGrady
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Wyy = Pac.T*self._Wyy*Pac
self._Wyy = Utils.sdiag((self.regmesh.vol*self.alpha_yy)**0.5)*self.regmesh.faceDiffy*self.regmesh.cellDiffy
return self._Wyy
@property
def Wzz(self):
"""Regularization matrix Wzz"""
if getattr(self, '_Wzz', None) is None:
self._Wzz = Utils.sdiag((self.mesh.vol*self.alpha_zz)**0.5)*self.mesh.faceDivz*self.mesh.cellGradz
if self.indActive is not None:
Pac = Utils.speye(self.mesh.nC)[:,self.indActive]
self._Wzz = Pac.T*self._Wzz*Pac
self._Wzz = Utils.sdiag((self.regmesh.vol*self.alpha_zz)**0.5)*self.regmesh.faceDiffz*self.regmesh.cellDiffz
return self._Wzz
@property
@@ -225,9 +498,9 @@ class Tikhonov(BaseRegularization):
"""Full smoothness regularization matrix W"""
if getattr(self, '_Wsmooth', None) is None:
wlist = (self.Wx, self.Wxx)
if self.mesh.dim > 1:
if self.regmesh.dim > 1:
wlist += (self.Wy, self.Wyy)
if self.mesh.dim > 2:
if self.regmesh.dim > 2:
wlist += (self.Wz, self.Wzz)
self._Wsmooth = sp.vstack(wlist)
return self._Wsmooth
@@ -236,25 +509,44 @@ class Tikhonov(BaseRegularization):
def W(self):
"""Full regularization matrix W"""
if getattr(self, '_W', None) is None:
wlist = (self.Ws, self.Wsmooth)
wlist = (self.Wsmall, self.Wsmooth)
self._W = sp.vstack(wlist)
return self._W
@Utils.timeIt
def eval(self, m):
if self.smoothModel == True:
r1 = self.Wsmooth * ( self.mapping * (m) )
r2 = self.Ws * ( self.mapping * (m - self.mref) )
return 0.5*(r1.dot(r1)+r2.dot(r2))
elif self.smoothModel == False:
r = self.W * ( self.mapping * (m - self.mref) )
return 0.5*r.dot(r)
def _evalSmall(self, m):
r = self.Wsmall * ( self.mapping * (m - self.mref) )
return 0.5 * r.dot(r)
@Utils.timeIt
def _evalSmooth(self, m):
if self.mrefInSmooth == True:
r = self.Wsmooth * ( self.mapping * (m - self.mref) )
elif self.mrefInSmooth == False:
r = self.Wsmooth * ( self.mapping * (m) )
return 0.5 * r.dot(r)
@Utils.timeIt
def eval(self, m):
return self._evalSmall(m) + self._evalSmooth(m)
@Utils.timeIt
def _evalSmallDeriv(self,m):
r = self.Wsmall * ( self.mapping * (m - self.mref) )
return r.T * ( self.Wsmall * self.mapping.deriv(m - self.mref) )
@Utils.timeIt
def _evalSmoothDeriv(self,m):
if self.mrefInSmooth == True:
r = self.Wsmooth * ( self.mapping * ( m - self.mref ) )
return r.T * ( self.Wsmooth * self.mapping.deriv(m - self.mref) )
elif self.mrefInSmooth == False:
r = self.Wsmooth * ( self.mapping * m )
return r.T * ( self.Wsmooth * self.mapping.deriv(m) )
@Utils.timeIt
def evalDeriv(self, m):
"""
The regularization is:
.. math::
@@ -268,17 +560,185 @@ class Tikhonov(BaseRegularization):
R(m) = \mathbf{W^\\top W (m-m_\\text{ref})}
"""
if self.smoothModel == True:
mD1 = self.mapping.deriv(m)
mD2 = self.mapping.deriv(m - self.mref)
r1 = self.Wsmooth * ( self.mapping * (m))
r2 = self.Ws * ( self.mapping * (m - self.mref) )
out1 = mD1.T * ( self.Wsmooth.T * r1 )
out2 = mD2.T * ( self.Ws.T * r2 )
out = out1+out2
elif self.smoothModel == False:
mD = self.mapping.deriv(m - self.mref)
r = self.W * ( self.mapping * (m - self.mref) )
out = mD.T * ( self.W.T * r )
return out
return self._evalSmallDeriv(m) + self._evalSmoothDeriv(m)
class Simple(Tikhonov):
"""
Simple regularization that does not include length scales in the derivatives.
"""
mrefInSmooth = False #: SMOOTH and SMOOTH_MOD_DIF options
alpha_s = Utils.dependentProperty('_alpha_s', 1.0, ['_W', '_Wsmall'], "Smallness weight")
alpha_x = Utils.dependentProperty('_alpha_x', 1.0, ['_W', '_Wx'], "Weight for the first derivative in the x direction")
alpha_y = Utils.dependentProperty('_alpha_y', 1.0, ['_W', '_Wy'], "Weight for the first derivative in the y direction")
alpha_z = Utils.dependentProperty('_alpha_z', 1.0, ['_W', '_Wz'], "Weight for the first derivative in the z direction")
wght = 1.
def __init__(self, mesh, mapping=None, indActive=None, **kwargs):
BaseRegularization.__init__(self, mesh, mapping=mapping, indActive=indActive, **kwargs)
if isinstance(self.wght,float):
self.wght = np.ones(self.regmesh.nC) * self.wght
@property
def Wsmall(self):
"""Regularization matrix Wsmall"""
if getattr(self,'_Wsmall', None) is None:
self._Wsmall = Utils.sdiag((self.regmesh.vol*self.alpha_s*self.wght)**0.5)
return self._Wsmall
@property
def Wx(self):
"""Regularization matrix Wx"""
if getattr(self, '_Wx', None) is None:
self._Wx = Utils.sdiag((self.regmesh.aveCC2Fx * self.regmesh.vol*self.alpha_x*(self.regmesh.aveCC2Fx*self.wght))**0.5)*self.regmesh.cellDiffxStencil
return self._Wx
@property
def Wy(self):
"""Regularization matrix Wy"""
if getattr(self, '_Wy', None) is None:
self._Wy = Utils.sdiag((self.regmesh.aveCC2Fy * self.regmesh.vol * self.alpha_y*(self.regmesh.aveCC2Fy*self.wght))**0.5)*self.regmesh.cellDiffyStencil
return self._Wy
@property
def Wz(self):
"""Regularization matrix Wz"""
if getattr(self, '_Wz', None) is None:
self._Wz = Utils.sdiag((self.regmesh.aveCC2Fz * self.regmesh.vol*self.alpha_z*(self.regmesh.aveCC2Fz*self.wght))**0.5)*self.regmesh.cellDiffzStencil
return self._Wz
@property
def Wsmooth(self):
"""Full smoothness regularization matrix W"""
if getattr(self, '_Wsmooth', None) is None:
wlist = (self.Wx,)
if self.regmesh.dim > 1:
wlist += (self.Wy,)
if self.regmesh.dim > 2:
wlist += (self.Wz,)
self._Wsmooth = sp.vstack(wlist)
return self._Wsmooth
@property
def W(self):
"""Full regularization matrix W"""
if getattr(self, '_W', None) is None:
wlist = (self.Wsmall, self.Wsmooth)
self._W = sp.vstack(wlist)
return self._W
@Utils.timeIt
def _evalSmall(self, m):
r = self.Wsmall * ( self.mapping * (m - self.mref) )
return 0.5 * r.dot(r)
@Utils.timeIt
def _evalSmooth(self, m):
if self.mrefInSmooth == True:
r = self.Wsmooth * ( self.mapping * (m - self.mref) )
elif self.mrefInSmooth == False:
r = self.Wsmooth * ( self.mapping * m)
return 0.5 * r.dot(r)
class Sparse(Simple):
# set default values
eps_p = 1e-1
eps_q = 1e-1
curModel = None # use a model to compute the weights
gamma = 1.
norms = [0., 2., 2., 2.]
wght = 1.
def __init__(self, mesh, mapping=None, indActive=None, **kwargs):
Simple.__init__(self, mesh, mapping=mapping, indActive=indActive, **kwargs)
if isinstance(self.wght,float):
self.wght = np.ones(self.regmesh.nC) * self.wght
@property
def Wsmall(self):
"""Regularization matrix Wsmall"""
if getattr(self, 'curModel', None) is None:
self.Rs = Utils.speye(self.regmesh.nC)
else:
f_m = self.curModel - self.reg.mref
self.rs = self.R(f_m , self.eps_p, self.norms[0])
#print "Min rs: " + str(np.max(self.rs)) + "Max rs: " + str(np.min(self.rs))
self.Rs = Utils.sdiag( self.rs )
return Utils.sdiag((self.regmesh.vol*self.alpha_s*self.gamma*self.wght)**0.5)*self.Rs
@property
def Wx(self):
"""Regularization matrix Wx"""
if getattr(self, 'curModel', None) is None:
self.Rx = Utils.speye(self.regmesh.cellDiffxStencil.shape[0])
else:
f_m = self.regmesh.cellDiffxStencil * self.curModel
self.rx = self.R( f_m , self.eps_q, self.norms[1])
self.Rx = Utils.sdiag( self.rx )
return Utils.sdiag(( (self.regmesh.aveCC2Fx * self.regmesh.vol) *self.alpha_x*self.gamma*(self.regmesh.aveCC2Fx*self.wght))**0.5)*self.Rx*self.regmesh.cellDiffxStencil
@property
def Wy(self):
"""Regularization matrix Wy"""
if getattr(self, 'curModel', None) is None:
self.Ry = Utils.speye(self.regmesh.cellDiffyStencil.shape[0])
else:
f_m = self.regmesh.cellDiffyStencil * self.curModel
self.ry = self.R( f_m , self.eps_q, self.norms[2])
self.Ry = Utils.sdiag( self.ry )
return Utils.sdiag(((self.regmesh.aveCC2Fy * self.regmesh.vol)*self.alpha_y*self.gamma*(self.regmesh.aveCC2Fy*self.wght))**0.5)*self.Ry*self.regmesh.cellDiffyStencil
@property
def Wz(self):
"""Regularization matrix Wz"""
if getattr(self, 'curModel', None) is None:
self.Rz = Utils.speye(self.regmesh.cellDiffzStencil.shape[0])
else:
f_m = self.regmesh.cellDiffzStencil * self.curModel
self.rz = self.R( f_m , self.eps_q, self.norms[3])
self.Rz = Utils.sdiag( self.rz )
return Utils.sdiag(((self.regmesh.aveCC2Fz * self.regmesh.vol)*self.alpha_z*self.gamma*(self.regmesh.aveCC2Fz*self.wght))**0.5)*self.Rz*self.regmesh.cellDiffzStencil
@property
def Wsmooth(self):
"""Full smoothness regularization matrix W"""
#if getattr(self, '_Wsmooth', None) is None:
wlist = (self.Wx,)
if self.regmesh.dim > 1:
wlist += (self.Wy,)
if self.regmesh.dim > 2:
wlist += (self.Wz,)
#self._Wsmooth = sp.vstack(wlist)
return sp.vstack(wlist)
@property
def W(self):
"""Full regularization matrix W"""
if getattr(self, '_W', None) is None:
wlist = (self.Wsmall, self.Wsmooth)
self._W = sp.vstack(wlist)
return self._W
def R(self, f_m , eps, exponent):
eta = (eps**(1.-exponent/2.))**0.5
r = eta / (f_m**2.+ eps**2.)**((1.-exponent/2.)/2.)
return r
+30 -20
View File
@@ -1,6 +1,5 @@
import Utils, numpy as np, scipy.sparse as sp, uuid
class BaseRx(object):
"""SimPEG Receiver Object"""
@@ -35,7 +34,7 @@ class BaseRx(object):
"""Number of data in the receiver."""
return self.locs.shape[0]
def getP(self, mesh):
def getP(self, mesh, projGLoc=None):
"""
Returns the projection matrices as a
list for all components collected by
@@ -48,7 +47,10 @@ class BaseRx(object):
if mesh in self._Ps:
return self._Ps[mesh]
P = mesh.getInterpolationMat(self.locs, self.projGLoc)
if projGLoc is None:
projGLoc = self.projGLoc
P = mesh.getInterpolationMat(self.locs, projGLoc)
if self.storeProjections:
self._Ps[mesh] = P
return P
@@ -293,38 +295,38 @@ class BaseSurvey(object):
@Utils.count
@Utils.requires('prob')
def dpred(self, m, u=None):
"""dpred(m, u=None)
def dpred(self, m, f=None):
"""dpred(m, f=None)
Create the projected data from a model.
The field, u, (if provided) will be used for the predicted data
The fields, f, (if provided) will be used for the predicted data
instead of recalculating the fields (which may be expensive!).
.. math::
d_\\text{pred} = P(u(m))
d_\\text{pred} = P(f(m))
Where P is a projection of the fields onto the data space.
"""
if u is None: u = self.prob.fields(m)
return Utils.mkvc(self.eval(u))
if f is None: f = self.prob.fields(m)
return Utils.mkvc(self.eval(f))
@Utils.count
def eval(self, u):
"""eval(u)
def eval(self, f):
"""eval(f)
This function projects the fields onto the data space.
.. math::
d_\\text{pred} = \mathbf{P} u(m)
d_\\text{pred} = \mathbf{P} f(m)
"""
raise NotImplemented('eval is not yet implemented.')
@Utils.count
def evalDeriv(self, u):
"""evalDeriv(u)
def evalDeriv(self, f):
"""evalDeriv(f)
This function s the derivative of projects the fields onto the data space.
@@ -335,11 +337,11 @@ class BaseSurvey(object):
raise NotImplemented('eval is not yet implemented.')
@Utils.count
def residual(self, m, u=None):
"""residual(m, u=None)
def residual(self, m, f=None):
"""residual(m, f=None)
:param numpy.array m: geophysical model
:param numpy.array u: fields
:param numpy.array f: fields
:rtype: numpy.array
:return: data residual
@@ -350,14 +352,14 @@ class BaseSurvey(object):
\mu_\\text{data} = \mathbf{d}_\\text{pred} - \mathbf{d}_\\text{obs}
"""
return Utils.mkvc(self.dpred(m, u=u) - self.dobs)
return Utils.mkvc(self.dpred(m, f=f) - self.dobs)
@property
def isSynthetic(self):
"Check if the data is synthetic."
return self.mtrue is not None
def makeSyntheticData(self, m, std=0.05, u=None, force=False):
def makeSyntheticData(self, m, std=0.05, f=None, force=False):
"""
Make synthetic data given a model, and a standard deviation.
@@ -370,8 +372,16 @@ class BaseSurvey(object):
if getattr(self, 'dobs', None) is not None and not force:
raise Exception('Survey already has dobs. You can use force=True to override this exception.')
self.mtrue = m
self.dtrue = self.dpred(m, u=u)
self.dtrue = self.dpred(m, f=f)
noise = std*abs(self.dtrue)*np.random.randn(*self.dtrue.shape)
self.dobs = self.dtrue+noise
self.std = self.dobs*0 + std
return self.dobs
class LinearSurvey(BaseSurvey):
def eval(self, f):
return f
@property
def nD(self):
return self.prob.G.shape[0]
+52 -4
View File
@@ -88,12 +88,14 @@ def getIndicesBlock(p0,p1,ccMesh):
# Return a tuple
return ind
def defineBlock(ccMesh,p0,p1,vals=[0,1]):
def defineBlock(ccMesh,p0,p1,vals=None):
"""
Build a block with the conductivity specified by condVal. Returns an array.
vals[0] conductivity of the block
vals[1] conductivity of the ground
"""
if vals is None:
vals = [0,1]
sigma = np.zeros(ccMesh.shape[0]) + vals[1]
ind = getIndicesBlock(p0,p1,ccMesh)
@@ -101,7 +103,11 @@ def defineBlock(ccMesh,p0,p1,vals=[0,1]):
return mkvc(sigma)
def defineElipse(ccMesh, center=[0,0,0], anisotropy=[1,1,1], slope=10., theta=0.):
def defineElipse(ccMesh, center=None, anisotropy=None, slope=10., theta=0.):
if center is None:
center = [0,0,0]
if anisotropy is None:
anisotropy = [1,1,1]
G = ccMesh.copy()
dim = ccMesh.shape[1]
for i in range(dim):
@@ -118,7 +124,45 @@ def defineElipse(ccMesh, center=[0,0,0], anisotropy=[1,1,1], slope=10., theta=0.
D = np.sqrt(np.sum(G**2,axis=1))
return -np.arctan((D-1)*slope)*(2./np.pi)/2.+0.5
def defineTwoLayers(ccMesh,depth,vals=[0,1]):
def getIndicesSphere(center,radius,ccMesh):
"""
Creates a vector containing the sphere indices in the cell centers mesh.
Returns a tuple
The sphere is defined by the points
p0, describe the position of the center of the cell
r, describe the radius of the sphere.
ccMesh represents the cell-centered mesh
The points p0 must live in the the same dimensional space as the mesh.
"""
# Validation: mesh and point (p0) live in the same dimensional space
dimMesh = np.size(ccMesh[0,:])
assert len(center) == dimMesh, "Dimension mismatch. len(p0) != dimMesh"
if dimMesh == 1:
# Define the reference points
ind = np.abs(center[0] - ccMesh[:,0]) < radius
elif dimMesh == 2:
# Define the reference points
ind = np.sqrt( ( center[0] - ccMesh[:,0] )**2 + ( center[1] - ccMesh[:,1] )**2 ) < radius
elif dimMesh == 3:
# Define the points
ind = np.sqrt( ( center[0] - ccMesh[:,0] )**2 + ( center[1] - ccMesh[:,1] )**2 + ( center[2] - ccMesh[:,2] )**2 ) < radius
# Return a tuple
return ind
def defineTwoLayers(ccMesh,depth,vals=None):
"""
Define a two layered model. Depth of the first layer must be specified.
CondVals vector with the conductivity values of the layers. Eg:
@@ -129,6 +173,8 @@ def defineTwoLayers(ccMesh,depth,vals=[0,1]):
0 depth zf
1st layer 2nd layer
"""
if vals is None:
vals = [0,1]
sigma = np.zeros(ccMesh.shape[0]) + vals[1]
dim = np.size(ccMesh[0,:])
@@ -214,7 +260,7 @@ def layeredModel(ccMesh, layerTops, layerValues):
def randomModel(shape, seed=None, anisotropy=None, its=100, bounds=[0,1]):
def randomModel(shape, seed=None, anisotropy=None, its=100, bounds=None):
"""
Create a random model by convolving a kernel with a
uniformly distributed model.
@@ -238,6 +284,8 @@ def randomModel(shape, seed=None, anisotropy=None, its=100, bounds=[0,1]):
"""
if bounds is None:
bounds = [0,1]
if seed is None:
seed = np.random.randint(1e3)
+3 -1
View File
@@ -55,8 +55,10 @@ def hook(obj, method, name=None, overwrite=False, silent=False):
print 'Method '+name+' was not overwritten.'
def setKwargs(obj, ignore=[], **kwargs):
def setKwargs(obj, ignore=None, **kwargs):
"""Sets key word arguments (kwargs) that are present in the object, throw an error if they don't exist."""
if ignore is None:
ignore = []
for attr in kwargs:
if attr in ignore:
continue
+137
View File
@@ -0,0 +1,137 @@
from SimPEG import np, Mesh
import time as tm
import vtk, vtk.util.numpy_support as npsup
import re
def read_GOCAD_ts(tsfile):
"""
Read GOCAD triangulated surface (*.ts) file
INPUT:
tsfile: Triangulated surface
OUTPUT:
vrts : Array of vertices in XYZ coordinates [n x 3]
trgl : Array of index for triangles [m x 3]. The order of the vertices
is important and describes the normal
n = cross( (P2 - P1 ) , (P3 - P1) )
Author: @fourndo
.. note::
Remove all attributes from the GoCAD surface before exporting it!
"""
fid = open(tsfile,'r')
line = fid.readline()
# Skip all the lines until the vertices
while re.match('TFACE',line)==None:
line = fid.readline()
line = fid.readline()
vrtx = []
# Run down all the vertices and save in array
while re.match('VRTX',line):
l_input = re.split('[\s*]',line)
temp = np.array(l_input[2:5])
vrtx.append(temp.astype(np.float))
# Read next line
line = fid.readline()
vrtx = np.asarray(vrtx)
# Skip lines to the triangles
while re.match('TRGL',line)==None:
line = fid.readline()
# Run down the list of triangles
trgl = []
# Run down all the vertices and save in array
while re.match('TRGL',line):
l_input = re.split('[\s*]',line)
temp = np.array(l_input[1:4])
trgl.append(temp.astype(np.int))
# Read next line
line = fid.readline()
trgl = np.asarray(trgl)
return vrtx, trgl
def surface2inds(vrtx, trgl, mesh, boundaries=True, internal=True):
""""
Function to read gocad polystructure file and output indexes of mesh with in the structure.
"""
# Adjust the index
trgl = trgl - 1
# Make vtk pts
ptsvtk = vtk.vtkPoints()
ptsvtk.SetData(npsup.numpy_to_vtk(vrtx,deep=1))
# Make the polygon connection
polys = vtk.vtkCellArray()
for face in trgl:
poly = vtk.vtkPolygon()
poly.GetPointIds().SetNumberOfIds(len(face))
for nrv, vert in enumerate(face):
poly.GetPointIds().SetId(nrv,vert)
polys.InsertNextCell(poly)
# Make the polydata, structure of connections and vrtx
polyData = vtk.vtkPolyData()
polyData.SetPoints(ptsvtk)
polyData.SetPolys(polys)
# Make implicit func
ImpDistFunc = vtk.vtkImplicitPolyDataDistance()
ImpDistFunc.SetInput(polyData)
# Convert the mesh
vtkMesh = vtk.vtkRectilinearGrid()
vtkMesh.SetDimensions(mesh.nNx,mesh.nNy,mesh.nNz)
vtkMesh.SetXCoordinates(npsup.numpy_to_vtk(mesh.vectorNx, deep=1))
vtkMesh.SetYCoordinates(npsup.numpy_to_vtk(mesh.vectorNy, deep=1))
vtkMesh.SetZCoordinates(npsup.numpy_to_vtk(mesh.vectorNz, deep=1))
# Add indexes
vtkInd = npsup.numpy_to_vtk(np.arange(mesh.nC), deep=1)
vtkInd.SetName('Index')
vtkMesh.GetCellData().AddArray(vtkInd)
extractImpDistRectGridFilt = vtk.vtkExtractGeometry() # Object constructor
extractImpDistRectGridFilt.SetImplicitFunction(ImpDistFunc) #
extractImpDistRectGridFilt.SetInputData(vtkMesh)
if boundaries is True:
extractImpDistRectGridFilt.ExtractBoundaryCellsOn()
else:
extractImpDistRectGridFilt.ExtractBoundaryCellsOff()
if internal is True:
extractImpDistRectGridFilt.ExtractInsideOn()
else:
extractImpDistRectGridFilt.ExtractInsideOff()
print "Extracting indices from grid..."
# Executing the pipe
extractImpDistRectGridFilt.Update()
# Get index inside
insideGrid = extractImpDistRectGridFilt.GetOutput()
insideGrid = npsup.vtk_to_numpy(insideGrid.GetCellData().GetArray('Index'))
# Return the indexes inside
return insideGrid
+1 -1
View File
@@ -15,7 +15,7 @@ import Directives
import Inversion
import Tests
__version__ = '0.1.9'
__version__ = '0.1.10'
__author__ = 'Rowan Cockett'
__license__ = 'MIT'
__copyright__ = 'Copyright 2014 Rowan Cockett'
+150
View File
@@ -0,0 +1,150 @@
.. _api_DC:
.. math::
\renewcommand{\div}{\nabla\cdot\,}
\newcommand{\grad}{\vec \nabla}
\newcommand{\curl}{{\vec \nabla}\times\,}
\newcommand{\dcurl}{{\mathbf C}}
\newcommand{\dgrad}{{\mathbf G}}
\newcommand{\Acf}{{\mathbf A_c^f}}
\newcommand{\Ace}{{\mathbf A_c^e}}
\renewcommand{\S}{{\mathbf \Sigma}}
\renewcommand{\Div}{{\mathbf {Div}}}
\renewcommand{\Grad}{{\mathbf {Grad}}}
\newcommand{\St}{{\mathbf \Sigma_\tau}}
\newcommand{\diag}{\mathbf{diag}}
\newcommand{\M}{{\mathbf M}}
\newcommand{\Me}{{\M^e}}
\newcommand{\Mes}[1]{{\M^e_{#1}}}
\newcommand{\be}{\mathbf{e}}
\newcommand{\bj}{\mathbf{j}}
\newcommand{\bphi}{\mathbf{\phi}}
\newcommand{\bq}{\mathbf{q}}
\newcommand{\bJ}{\mathbf{J}}
\newcommand{\bG}{\mathbf{G}}
\newcommand{\bP}{\mathbf{P}}
\newcommand{\bA}{\mathbf{A}}
\newcommand{\bm}{\mathbf{m}}
\newcommand{\B}{\vec{B}}
\newcommand{\D}{\vec{D}}
\renewcommand{\H}{\vec{H}}
\renewcommand {\j} { {\vec j} }
\newcommand {\h} { {\vec h} }
\renewcommand {\b} { {\vec b} }
\newcommand {\e} { {\vec e} }
\newcommand {\c} { {\vec c} }
\renewcommand {\d} { {\vec d} }
\renewcommand {\u} { {\vec u} }
\newcommand{\I}{\vec{I}}
DC resistivity survey
*********************
Electrical resistivity of subsurface materials is measured by causing an electrical current to flow in the earth between one pair of electrodes while the voltage across a second pair of electrodes is measured. The result is an "apparent" resistivity which is a value representing the weighted average resistivity over a volume of the earth. Variations in this measurement are caused by variations in the soil, rock, and pore fluid electrical resistivity. Surveys require contact with the ground, so they can be labour intensive. Results are sometimes interpreted directly, but more commonly, 1D, 2D or 3D models are estimated using inversion procedures (`GPG <http://www.eos.ubc.ca/courses/eosc350/content/>`_).
Background
==========
As direct current (DC) implies, in DC resistivity survey, we assume steady-state. We consider Maxwell's equations in steady state as
.. math::
\curl \frac{1}{\mu} \vec{b} - \j = \j_s \\
\curl \e = 0
Then by taking \\(\\curl\\) for the first equation, we have
.. math::
- \div\j = q \\
where
.. math::
\div \j_s = q = I(\delta(\vec{r}-\vec{r}_{s+})-\delta(\vec{r}-\vec{r}_{s-}))
Since \\(\\curl \\e = 0\\), we have
.. math::
\e = \grad \phi
And by Ohm's law, we have
.. math::
\j = \sigma \grad \phi
Finally, we can compute the solution of the system:
.. math::
- \div\j = q
\j = \sigma \grad \phi
\frac{\partial \phi}{\partial r}\Big|_{\partial \Omega_{BC}} = 0
Discretization
==============
By using finite volume method (FVM), we discretize our system as
.. math::
-\Div \bj = \bq
\diag(\Acf^{T}\sigma^{-1}) \bj = \Grad \bphi
Here boundary condtions are embedded in the discrete differential operators. With some linear algebra we have
.. math::
\bA\bphi = -\bq
where
.. math::
\bA = \Div (\diag(\Acf^{T}\sigma^{-1}))^{-1} \Grad
By solving this linear equation, we can compute the solution of \\(\\phi\\). Based on this discretization, we derive sensitivity in discretized space. Sensitivity matrix can be in general can be written as
.. math ::
\bJ = -\bP\bA^{-1}\bG
where
.. math ::
\bP: \text{Projection}
\bJ = \bP\frac{\partial \phi}{\partial \bm}
Here \\(\\bm\\) indicates model parameters in discretized space.
Verification
============
Comparing to the analytic function:
.. plot::
import simpegDC as DC
DC.Examples.Verification.run(plotIt=True)
API
===
.. automodule:: simpegDC.BaseDC
:show-inheritance:
:members:
:undoc-members:
:inherited-members:
+2 -2
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@@ -51,9 +51,9 @@ copyright = u'2013, SimPEG Developers'
# built documents.
#
# The short X.Y version.
version = '0.1.9'
version = '0.1.10'
# The full version, including alpha/beta/rc tags.
release = '0.1.9'
release = '0.1.10'
# The language for content autogenerated by Sphinx. Refer to documentation
# for a list of supported languages.
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@@ -0,0 +1,21 @@
.. _examples_DC_Analytic_Dipole:
.. --------------------------------- ..
.. ..
.. THIS FILE IS AUTO GENEREATED ..
.. ..
.. SimPEG/Examples/__init__.py ..
.. ..
.. --------------------------------- ..
DC Analytic Dipole
==================
.. plot::
from SimPEG import Examples
Examples.DC_Analytic_Dipole.run()
.. literalinclude:: ../../SimPEG/Examples/DC_Analytic_Dipole.py
:language: python
:linenos:
@@ -0,0 +1,36 @@
.. _examples_DC_Forward_PseudoSection:
.. --------------------------------- ..
.. ..
.. THIS FILE IS AUTO GENEREATED ..
.. ..
.. SimPEG/Examples/__init__.py ..
.. ..
.. --------------------------------- ..
DC Forward Simulation
=====================
Forward model two conductive spheres in a half-space and plot a
pseudo-section. Assumes an infinite line source and measures along the
center of the spheres.
INPUT:
loc = Location of spheres [[x1,y1,z1],[x2,y2,z2]]
radi = Radius of spheres [r1,r2]
param = Conductivity of background and two spheres [m0,m1,m2]
stype = survey type "pdp" (pole dipole) or "dpdp" (dipole dipole)
dtype = Data type "appr" (app res) | "appc" (app cond) | "volt" (potential)
Created by @fourndo
.. plot::
from SimPEG import Examples
Examples.DC_Forward_PseudoSection.run()
.. literalinclude:: ../../SimPEG/Examples/DC_Forward_PseudoSection.py
:language: python
:linenos:
@@ -0,0 +1,58 @@
.. _examples_EM_Schenkel_Morrison_Casing:
.. --------------------------------- ..
.. ..
.. THIS FILE IS AUTO GENEREATED ..
.. ..
.. SimPEG/Examples/__init__.py ..
.. ..
.. --------------------------------- ..
EM: Schenkel and Morrison Casing Model
======================================
Here we create and run a FDEM forward simulation to calculate the vertical
current inside a steel-cased. The model is based on the Schenkel and
Morrison Casing Model, and the results are used in a 2016 SEG abstract by
Yang et al.
- Schenkel, C.J., and H.F. Morrison, 1990, Effects of well casing on potential field measurements using downhole current sources: Geophysical prospecting, 38, 663-686.
The model consists of:
- Air: Conductivity 1e-8 S/m, above z = 0
- Background: conductivity 1e-2 S/m, below z = 0
- Casing: conductivity 1e6 S/m
- 300m long
- radius of 0.1m
- thickness of 6e-3m
Inside the casing, we take the same conductivity as the background.
We are using an EM code to simulate DC, so we use frequency low enough
that the skin depth inside the casing is longer than the casing length (f
= 1e-6 Hz). The plot produced is of the current inside the casing.
These results are shown in the SEG abstract by Yang et al., 2016: 3D DC
resistivity modeling of steel casing for reservoir monitoring using
equivalent resistor network. The solver used to produce these results and
achieve the CPU time of ~30s is Mumps, which was installed using pymatsolver_
.. _pymatsolver: https://github.com/rowanc1/pymatsolver
This example is on figshare: https://dx.doi.org/10.6084/m9.figshare.3126961.v1
If you would use this example for a code comparison, or build upon it, a
citation would be much appreciated!
.. plot::
from SimPEG import Examples
Examples.EM_Schenkel_Morrison_Casing.run()
.. literalinclude:: ../../SimPEG/Examples/EM_Schenkel_Morrison_Casing.py
:language: python
:linenos:
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@@ -0,0 +1,26 @@
.. _examples_Inversion_IRLS:
.. --------------------------------- ..
.. ..
.. THIS FILE IS AUTO GENEREATED ..
.. ..
.. SimPEG/Examples/__init__.py ..
.. ..
.. --------------------------------- ..
Inversion: Linear Problem
=========================
Here we go over the basics of creating a linear problem and inversion.
.. plot::
from SimPEG import Examples
Examples.Inversion_IRLS.run()
.. literalinclude:: ../../SimPEG/Examples/Inversion_IRLS.py
:language: python
:linenos:
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@@ -77,7 +77,7 @@ with open("README.rst") as f:
setup(
name = "SimPEG",
version = "0.1.9",
version = "0.1.10",
packages = find_packages(),
install_requires = ['numpy>=1.7',
'scipy>=0.13',
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@@ -5,6 +5,8 @@ from scipy.sparse.linalg import dsolve
import inspect
TOL = 1e-20
testReg = True
testRegMesh = True
class RegularizationTests(unittest.TestCase):
@@ -16,44 +18,80 @@ class RegularizationTests(unittest.TestCase):
mesh3 = Mesh.TensorMesh([hx, hy, hz])
self.meshlist = [mesh1,mesh2, mesh3]
def test_regularization(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
if testReg:
def test_regularization(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
for i, mesh in enumerate(self.meshlist):
print 'Testing %iD'%mesh.dim
mapping = r.mapPair(mesh)
reg = r(mesh, mapping=mapping)
m = np.random.rand(mapping.nP)
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
def test_regularization_ActiveCells(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
for i, mesh in enumerate(self.meshlist):
print 'Testing Active Cells %iD'%(mesh.dim)
if mesh.dim == 1:
indActive = Utils.mkvc(mesh.gridCC <= 0.8)
elif mesh.dim == 2:
indActive = Utils.mkvc(mesh.gridCC[:,-1] <= 2*np.sin(2*np.pi*mesh.gridCC[:,0])+0.5)
elif mesh.dim == 3:
indActive = Utils.mkvc(mesh.gridCC[:,-1] <= 2*np.sin(2*np.pi*mesh.gridCC[:,0])+0.5 * 2*np.sin(2*np.pi*mesh.gridCC[:,1])+0.5)
for indAct in [indActive, indActive.nonzero()[0]]: # test both bool and integers
reg = r(mesh, indActive=indAct)
m = np.random.rand(mesh.nC)[indAct]
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
if testRegMesh:
def test_regularizationMesh(self):
for i, mesh in enumerate(self.meshlist):
print 'Testing %iD'%mesh.dim
mapping = r.mapPair(mesh)
reg = r(mesh, mapping=mapping)
m = np.random.rand(mapping.nP)
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
def test_regularization_ActiveCells(self):
for R in dir(Regularization):
r = getattr(Regularization, R)
if not inspect.isclass(r): continue
if not issubclass(r, Regularization.BaseRegularization):
continue
for i, mesh in enumerate(self.meshlist):
print 'Testing Active Cells %iD'%(mesh.dim)
# mapping = r.mapPair(mesh)
# reg = r(mesh, mapping=mapping)
# m = np.random.rand(mapping.nP)
if mesh.dim == 1:
indAct = Utils.mkvc(mesh.gridCC <= 0.8)
@@ -62,23 +100,9 @@ class RegularizationTests(unittest.TestCase):
elif mesh.dim == 3:
indAct = Utils.mkvc(mesh.gridCC[:,-1] <= 2*np.sin(2*np.pi*mesh.gridCC[:,0])+0.5 * 2*np.sin(2*np.pi*mesh.gridCC[:,1])+0.5)
mapping = Maps.IdentityMap(nP=indAct.nonzero()[0].size)
regmesh = Regularization.RegularizationMesh(mesh, indActive=indAct)
reg = r(mesh, mapping=mapping, indActive=indAct)
m = np.random.rand(mesh.nC)[indAct]
reg.mref = np.ones_like(m)*np.mean(m)
print 'Check: phi_m (mref) = %f' %reg.eval(reg.mref)
passed = reg.eval(reg.mref) < TOL
self.assertTrue(passed)
print 'Check:', R
passed = Tests.checkDerivative(lambda m : [reg.eval(m), reg.evalDeriv(m)], m, plotIt=False)
self.assertTrue(passed)
print 'Check 2 Deriv:', R
passed = Tests.checkDerivative(lambda m : [reg.evalDeriv(m), reg.eval2Deriv(m)], m, plotIt=False)
self.assertTrue(passed)
assert (regmesh.vol == mesh.vol[indAct]).all()
if __name__ == '__main__':
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@@ -0,0 +1,12 @@
import os
import glob
import unittest
if __name__ == '__main__':
test_file_strings = glob.glob('test_*.py')
module_strings = [str[0:len(str)-3] for str in test_file_strings]
suites = [unittest.defaultTestLoader.loadTestsFromName(str) for str
in module_strings]
testSuite = unittest.TestSuite(suites)
unittest.TextTestRunner(verbosity=2).run(testSuite)
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@@ -0,0 +1,77 @@
import unittest
from SimPEG import *
import SimPEG.DCIP as DC
class DCProblemTests(unittest.TestCase):
def setUp(self):
aSpacing=2.5
nElecs=10
surveySize = nElecs*aSpacing - aSpacing
cs = surveySize/nElecs/4
mesh = Mesh.TensorMesh([
[(cs,10, -1.3),(cs,surveySize/cs),(cs,10, 1.3)],
[(cs,3, -1.3),(cs,3,1.3)],
# [(cs,5, -1.3),(cs,10)]
],'CN')
srcList = DC.Utils.WennerSrcList(nElecs, aSpacing, in2D=True)
survey = DC.SurveyDC(srcList)
problem = DC.ProblemDC_CC(mesh)
problem.pair(survey)
mSynth = np.ones(mesh.nC)
survey.makeSyntheticData(mSynth)
# Now set up the problem to do some minimization
dmis = DataMisfit.l2_DataMisfit(survey)
reg = Regularization.Tikhonov(mesh)
opt = Optimization.InexactGaussNewton(maxIterLS=20, maxIter=10, tolF=1e-6, tolX=1e-6, tolG=1e-6, maxIterCG=6)
invProb = InvProblem.BaseInvProblem(dmis, reg, opt, beta=1e4)
inv = Inversion.BaseInversion(invProb)
self.inv = inv
self.reg = reg
self.p = problem
self.mesh = mesh
self.m0 = mSynth
self.survey = survey
self.dmis = dmis
def test_misfit(self):
derChk = lambda m: [self.survey.dpred(m), lambda mx: self.p.Jvec(self.m0, mx)]
passed = Tests.checkDerivative(derChk, self.m0, plotIt=False)
self.assertTrue(passed)
def test_adjoint(self):
# Adjoint Test
u = np.random.rand(self.mesh.nC*self.survey.nSrc)
v = np.random.rand(self.mesh.nC)
w = np.random.rand(self.survey.dobs.shape[0])
wtJv = w.dot(self.p.Jvec(self.m0, v))
vtJtw = v.dot(self.p.Jtvec(self.m0, w))
passed = np.abs(wtJv - vtJtw) < 1e-10
print 'Adjoint Test', np.abs(wtJv - vtJtw), passed
self.assertTrue(passed)
def test_dataObj(self):
derChk = lambda m: [self.dmis.eval(m), self.dmis.evalDeriv(m)]
passed = Tests.checkDerivative(derChk, self.m0, plotIt=False)
self.assertTrue(passed)
def test_massMatrices(self):
Gu = np.random.rand(self.mesh.nF)
def derChk(m):
self.p.curModel = m
return [self.p.Msig * Gu, self.p.dMdsig(Gu)]
passed = Tests.checkDerivative(derChk, self.m0, plotIt=False)
self.assertTrue(passed)
if __name__ == '__main__':
unittest.main()
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@@ -0,0 +1,65 @@
import unittest
import SimPEG.DCIP as DC
from SimPEG import *
class IPforwardTests(unittest.TestCase):
def test_IPforward(self):
cs = 12.5
nc = 200/cs+1
hx = [(cs,7, -1.3),(cs,nc),(cs,7, 1.3)]
hy = [(cs,7, -1.3),(cs,int(nc/2+1)),(cs,7, 1.3)]
hz = [(cs,7, -1.3),(cs,int(nc/2+1))]
mesh = Mesh.TensorMesh([hx, hy, hz], 'CCN')
sighalf = 1e-2
sigma = np.ones(mesh.nC)*sighalf
p0 = np.r_[-50., 50., -50.]
p1 = np.r_[ 50.,-50., -150.]
blk_ind = Utils.ModelBuilder.getIndicesBlock(p0, p1, mesh.gridCC)
sigma[blk_ind] = 1e-3
eta = np.zeros_like(sigma)
eta[blk_ind] = 0.1
sigmaInf = sigma.copy()
sigma0 = sigma*(1-eta)
nElecs = 11
x_temp = np.linspace(-100, 100, nElecs)
aSpacing = x_temp[1]-x_temp[0]
y_temp = 0.
xyz = Utils.ndgrid(x_temp, np.r_[y_temp], np.r_[0.])
srcList = DC.Utils.WennerSrcList(nElecs,aSpacing)
survey = DC.SurveyDC(srcList)
imap = Maps.IdentityMap(mesh)
problem = DC.ProblemDC_CC(mesh, mapping=imap)
try:
from pymatsolver import MumpsSolver
solver = MumpsSolver
except ImportError, e:
solver = SolverLU
problem.Solver = solver
problem.pair(survey)
phi0 = survey.dpred(sigma0)
phiInf = survey.dpred(sigmaInf)
phiIP_true = phi0-phiInf
surveyIP = DC.SurveyIP(srcList)
problemIP = DC.ProblemIP(mesh, sigma=sigma)
problemIP.pair(surveyIP)
problemIP.Solver = solver
phiIP_approx = surveyIP.dpred(eta)
err = np.linalg.norm(phiIP_true-phiIP_approx) / np.linalg.norm(phiIP_true)
self.assertTrue(err < 0.02)
if __name__ == '__main__':
unittest.main()
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@@ -0,0 +1,82 @@
import unittest
from SimPEG import *
import SimPEG.DCIP as DC
class IPProblemTests(unittest.TestCase):
def setUp(self):
cs = 12.5
nc = 500/cs+1
hx = [(cs,0, -1.3),(cs,nc),(cs,0, 1.3)]
hy = [(cs,0, -1.3),(cs,int(nc/2+1)),(cs,0, 1.3)]
hz = [(cs,0, -1.3),(cs,int(nc/2+1))]
mesh = Mesh.TensorMesh([hx, hy, hz], 'CCN')
sighalf = 1e-2
sigma = np.ones(mesh.nC)*sighalf
p0 = np.r_[-50., 50., -50.]
p1 = np.r_[ 50.,-50., -150.]
blk_ind = Utils.ModelBuilder.getIndicesBlock(p0, p1, mesh.gridCC)
sigma[blk_ind] = 1e-3
eta = np.zeros_like(sigma)
eta[blk_ind] = 0.1
nElecs = 5
x_temp = np.linspace(-250, 250, nElecs)
aSpacing = x_temp[1]-x_temp[0]
y_temp = 0.
xyz = Utils.ndgrid(x_temp, np.r_[y_temp], np.r_[0.])
srcList = DC.Utils.WennerSrcList(nElecs,aSpacing)
survey = DC.SurveyIP(srcList)
imap = Maps.IdentityMap(mesh)
problem = DC.ProblemIP(mesh, sigma=sigma, mapping= imap)
problem.pair(survey)
try:
from pymatsolver import MumpsSolver
problem.Solver = MumpsSolver
except ImportError, e:
problem.Solver = SolverLU
mSynth = eta
survey.makeSyntheticData(mSynth)
# Now set up the problem to do some minimization
dmis = DataMisfit.l2_DataMisfit(survey)
reg = Regularization.Tikhonov(mesh)
opt = Optimization.InexactGaussNewton(maxIterLS=20, maxIter=10, tolF=1e-6, tolX=1e-6, tolG=1e-6, maxIterCG=6)
invProb = InvProblem.BaseInvProblem(dmis, reg, opt, beta=1e4)
inv = Inversion.BaseInversion(invProb)
self.inv = inv
self.reg = reg
self.p = problem
self.mesh = mesh
self.m0 = mSynth
self.survey = survey
self.dmis = dmis
def test_misfit(self):
derChk = lambda m: [self.survey.dpred(m), lambda mx: self.p.Jvec(self.m0, mx)]
passed = Tests.checkDerivative(derChk, self.m0*0, plotIt=False)
self.assertTrue(passed)
def test_adjoint(self):
# Adjoint Test
u = np.random.rand(self.mesh.nC*self.survey.nSrc)
v = np.random.rand(self.mesh.nC)
w = np.random.rand(self.survey.dobs.shape[0])
wtJv = w.dot(self.p.Jvec(self.m0, v))
vtJtw = v.dot(self.p.Jtvec(self.m0, w))
passed = np.abs(wtJv - vtJtw) < 1e-10
print 'Adjoint Test', np.abs(wtJv - vtJtw), passed
self.assertTrue(passed)
def test_dataObj(self):
derChk = lambda m: [self.dmis.eval(m), self.dmis.evalDeriv(m)]
passed = Tests.checkDerivative(derChk, self.m0, plotIt=False)
self.assertTrue(passed)
if __name__ == '__main__':
unittest.main()
+4 -4
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@@ -28,12 +28,12 @@ class FDEM_analyticTests(unittest.TestCase):
x = np.linspace(-10,10,5)
XYZ = Utils.ndgrid(x,np.r_[0],np.r_[0])
rxList = EM.FDEM.Rx(XYZ, 'exi')
rxList = EM.FDEM.Rx.eField(XYZ, orientation='x', real_or_imag='imag')
Src0 = EM.FDEM.Src.MagDipole([rxList],loc=np.r_[0.,0.,0.], freq=freq)
survey = EM.FDEM.Survey([Src0])
prb = EM.FDEM.Problem_b(mesh, mapping=mapping)
prb = EM.FDEM.Problem3D_b(mesh, mapping=mapping)
prb.pair(survey)
try:
@@ -125,8 +125,8 @@ class FDEM_analyticTests(unittest.TestCase):
mapping = [('sigma', Maps.IdentityMap(mesh)),('mu', Maps.IdentityMap(mesh))]
prbe = EM.FDEM.Problem_h(mesh, mapping=mapping)
prbm = EM.FDEM.Problem_e(mesh, mapping=mapping)
prbe = EM.FDEM.Problem3D_h(mesh, mapping=mapping)
prbm = EM.FDEM.Problem3D_e(mesh, mapping=mapping)
prbe.pair(surveye) # pair problem and survey
prbm.pair(surveym)
+30 -80
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@@ -3,125 +3,75 @@ from SimPEG import *
from SimPEG import EM
import sys
from scipy.constants import mu_0
from SimPEG.EM.Utils.testingUtils import getFDEMProblem
from SimPEG.EM.Utils.testingUtils import getFDEMProblem, crossCheckTest
testEB = True
testHJ = True
testEJ = True
testBH = True
verbose = False
TOL = 1e-5
FLR = 1e-20 # "zero", so if residual below this --> pass regardless of order
CONDUCTIVITY = 1e1
MU = mu_0
freq = 1e-1
addrandoms = True
TOLEBHJ = 1e-5
TOLEJHB = 1 # averaging and more sensitive to boundary condition violations (ie. the impact of violating the boundary conditions in each case is different.)
#TODO: choose better testing parameters to lower this
SrcList = ['RawVec', 'MagDipole_Bfield', 'MagDipole', 'CircularLoop']
def crossCheckTest(fdemType, comp):
l2norm = lambda r: np.sqrt(r.dot(r))
prb1 = getFDEMProblem(fdemType, comp, SrcList, freq, verbose)
mesh = prb1.mesh
print 'Cross Checking Forward: %s formulation - %s' % (fdemType, comp)
m = np.log(np.ones(mesh.nC)*CONDUCTIVITY)
mu = np.log(np.ones(mesh.nC)*MU)
if addrandoms is True:
m = m + np.random.randn(mesh.nC)*np.log(CONDUCTIVITY)*1e-1
mu = mu + np.random.randn(mesh.nC)*MU*1e-1
# prb1.PropMap.PropModel.mu = mu
# prb1.PropMap.PropModel.mui = 1./mu
survey1 = prb1.survey
d1 = survey1.dpred(m)
if verbose:
print ' Problem 1 solved'
if fdemType == 'e':
prb2 = getFDEMProblem('b', comp, SrcList, freq, verbose)
elif fdemType == 'b':
prb2 = getFDEMProblem('e', comp, SrcList, freq, verbose)
elif fdemType == 'j':
prb2 = getFDEMProblem('h', comp, SrcList, freq, verbose)
elif fdemType == 'h':
prb2 = getFDEMProblem('j', comp, SrcList, freq, verbose)
else:
raise NotImplementedError()
# prb2.mu = mu
survey2 = prb2.survey
d2 = survey2.dpred(m)
if verbose:
print ' Problem 2 solved'
r = d2-d1
l2r = l2norm(r)
tol = np.max([TOL*(10**int(np.log10(l2norm(d1)))),FLR])
print l2norm(d1), l2norm(d2), l2r , tol, l2r < tol
return l2r < tol
class FDEM_CrossCheck(unittest.TestCase):
if testEB:
def test_EB_CrossCheck_exr_Eform(self):
self.assertTrue(crossCheckTest('e', 'exr'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'exr', verbose=verbose))
def test_EB_CrossCheck_eyr_Eform(self):
self.assertTrue(crossCheckTest('e', 'eyr'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'eyr', verbose=verbose))
def test_EB_CrossCheck_ezr_Eform(self):
self.assertTrue(crossCheckTest('e', 'ezr'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'ezr', verbose=verbose))
def test_EB_CrossCheck_exi_Eform(self):
self.assertTrue(crossCheckTest('e', 'exi'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'exi', verbose=verbose))
def test_EB_CrossCheck_eyi_Eform(self):
self.assertTrue(crossCheckTest('e', 'eyi'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'eyi', verbose=verbose))
def test_EB_CrossCheck_ezi_Eform(self):
self.assertTrue(crossCheckTest('e', 'ezi'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'ezi', verbose=verbose))
def test_EB_CrossCheck_bxr_Eform(self):
self.assertTrue(crossCheckTest('e', 'bxr'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'bxr', verbose=verbose))
def test_EB_CrossCheck_byr_Eform(self):
self.assertTrue(crossCheckTest('e', 'byr'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'byr', verbose=verbose))
def test_EB_CrossCheck_bzr_Eform(self):
self.assertTrue(crossCheckTest('e', 'bzr'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'bzr', verbose=verbose))
def test_EB_CrossCheck_bxi_Eform(self):
self.assertTrue(crossCheckTest('e', 'bxi'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'bxi', verbose=verbose))
def test_EB_CrossCheck_byi_Eform(self):
self.assertTrue(crossCheckTest('e', 'byi'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'byi', verbose=verbose))
def test_EB_CrossCheck_bzi_Eform(self):
self.assertTrue(crossCheckTest('e', 'bzi'))
self.assertTrue(crossCheckTest(SrcList, 'e', 'b', 'bzi', verbose=verbose))
if testHJ:
def test_HJ_CrossCheck_jxr_Jform(self):
self.assertTrue(crossCheckTest('j', 'jxr'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'jxr', verbose=verbose))
def test_HJ_CrossCheck_jyr_Jform(self):
self.assertTrue(crossCheckTest('j', 'jyr'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'jyr', verbose=verbose))
def test_HJ_CrossCheck_jzr_Jform(self):
self.assertTrue(crossCheckTest('j', 'jzr'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'jzr', verbose=verbose))
def test_HJ_CrossCheck_jxi_Jform(self):
self.assertTrue(crossCheckTest('j', 'jxi'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'jxi', verbose=verbose))
def test_HJ_CrossCheck_jyi_Jform(self):
self.assertTrue(crossCheckTest('j', 'jyi'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'jyi', verbose=verbose))
def test_HJ_CrossCheck_jzi_Jform(self):
self.assertTrue(crossCheckTest('j', 'jzi'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'jzi', verbose=verbose))
def test_HJ_CrossCheck_hxr_Jform(self):
self.assertTrue(crossCheckTest('j', 'hxr'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'hxr', verbose=verbose))
def test_HJ_CrossCheck_hyr_Jform(self):
self.assertTrue(crossCheckTest('j', 'hyr'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'hyr', verbose=verbose))
def test_HJ_CrossCheck_hzr_Jform(self):
self.assertTrue(crossCheckTest('j', 'hzr'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'hzr', verbose=verbose))
def test_HJ_CrossCheck_hxi_Jform(self):
self.assertTrue(crossCheckTest('j', 'hxi'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'hxi', verbose=verbose))
def test_HJ_CrossCheck_hyi_Jform(self):
self.assertTrue(crossCheckTest('j', 'hyi'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'hyi', verbose=verbose))
def test_HJ_CrossCheck_hzi_Jform(self):
self.assertTrue(crossCheckTest('j', 'hzi'))
self.assertTrue(crossCheckTest(SrcList, 'j', 'h', 'hzi', verbose=verbose))
if __name__ == '__main__':
unittest.main()
@@ -0,0 +1,125 @@
import unittest
from SimPEG import *
from SimPEG import EM
import sys
from scipy.constants import mu_0
from SimPEG.EM.Utils.testingUtils import getFDEMProblem, crossCheckTest
testEJ = True
testBH = True
TOLEJHB = 1 # averaging and more sensitive to boundary condition violations (ie. the impact of violating the boundary conditions in each case is different.)
#TODO: choose better testing parameters to lower this
SrcList = ['RawVec', 'MagDipole', 'MagDipole_Bfield', 'MagDipole', 'CircularLoop']
class FDEM_CrossCheck(unittest.TestCase):
if testEJ:
def test_EJ_CrossCheck_jxr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'jxr', TOL=TOLEJHB))
def test_EJ_CrossCheck_jyr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'jyr', TOL=TOLEJHB))
def test_EJ_CrossCheck_jzr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'jzr', TOL=TOLEJHB))
def test_EJ_CrossCheck_jxi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'jxi', TOL=TOLEJHB))
def test_EJ_CrossCheck_jyi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'jyi', TOL=TOLEJHB))
def test_EJ_CrossCheck_jzi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'jzi', TOL=TOLEJHB))
def test_EJ_CrossCheck_exr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'exr', TOL=TOLEJHB))
def test_EJ_CrossCheck_eyr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'eyr', TOL=TOLEJHB))
def test_EJ_CrossCheck_ezr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'ezr', TOL=TOLEJHB))
def test_EJ_CrossCheck_exi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'exi', TOL=TOLEJHB))
def test_EJ_CrossCheck_eyi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'eyi', TOL=TOLEJHB))
def test_EJ_CrossCheck_ezi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'ezi', TOL=TOLEJHB))
def test_EJ_CrossCheck_bxr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'bxr', TOL=TOLEJHB))
def test_EJ_CrossCheck_byr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'byr', TOL=TOLEJHB))
def test_EJ_CrossCheck_bzr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'bzr', TOL=TOLEJHB))
def test_EJ_CrossCheck_bxi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'bxi', TOL=TOLEJHB))
def test_EJ_CrossCheck_byi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'byi', TOL=TOLEJHB))
def test_EJ_CrossCheck_bzi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'bzi', TOL=TOLEJHB))
def test_EJ_CrossCheck_hxr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'hxr', TOL=TOLEJHB))
def test_EJ_CrossCheck_hyr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'hyr', TOL=TOLEJHB))
def test_EJ_CrossCheck_hzr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'hzr', TOL=TOLEJHB))
def test_EJ_CrossCheck_hxi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'hxi', TOL=TOLEJHB))
def test_EJ_CrossCheck_hyi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'hyi', TOL=TOLEJHB))
def test_EJ_CrossCheck_hzi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'e', 'j', 'hzi', TOL=TOLEJHB))
if testBH:
def test_HB_CrossCheck_jxr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'jxr', TOL=TOLEJHB))
def test_HB_CrossCheck_jyr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'jyr', TOL=TOLEJHB))
def test_HB_CrossCheck_jzr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'jzr', TOL=TOLEJHB))
def test_HB_CrossCheck_jxi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'jxi', TOL=TOLEJHB))
def test_HB_CrossCheck_jyi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'jyi', TOL=TOLEJHB))
def test_HB_CrossCheck_jzi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'jzi', TOL=TOLEJHB))
def test_HB_CrossCheck_exr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'exr', TOL=TOLEJHB))
def test_HB_CrossCheck_eyr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'eyr', TOL=TOLEJHB))
def test_HB_CrossCheck_ezr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'ezr', TOL=TOLEJHB))
def test_HB_CrossCheck_exi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'exi', TOL=TOLEJHB))
def test_HB_CrossCheck_eyi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'eyi', TOL=TOLEJHB))
def test_HB_CrossCheck_ezi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'ezi', TOL=TOLEJHB))
def test_HB_CrossCheck_bxr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'bxr', TOL=TOLEJHB))
def test_HB_CrossCheck_byr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'byr', TOL=TOLEJHB))
def test_HB_CrossCheck_bzr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'bzr', TOL=TOLEJHB))
def test_HB_CrossCheck_bxi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'bxi', TOL=TOLEJHB))
def test_HB_CrossCheck_byi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'byi', TOL=TOLEJHB))
def test_HB_CrossCheck_bzi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'bzi', TOL=TOLEJHB))
def test_HB_CrossCheck_hxr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'hxr', TOL=TOLEJHB))
def test_HB_CrossCheck_hyr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'hyr', TOL=TOLEJHB))
def test_HB_CrossCheck_hzr_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'hzr', TOL=TOLEJHB))
def test_HB_CrossCheck_hxi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'hxi', TOL=TOLEJHB))
def test_HB_CrossCheck_hyi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'hyi', TOL=TOLEJHB))
def test_HB_CrossCheck_hzi_Jform(self):
self.assertTrue(crossCheckTest(SrcList, 'h', 'b', 'hzi', TOL=TOLEJHB))
if __name__ == '__main__':
unittest.main()
@@ -0,0 +1,128 @@
import unittest
from SimPEG import *
from SimPEG import EM
import sys
from scipy.constants import mu_0
from SimPEG.EM.Utils.testingUtils import getFDEMProblem, crossCheckTest
testEB = True
testHJ = True
testEJ = True
testBH = True
verbose = False
TOLEJHB = 1 # averaging and more sensitive to boundary condition violations (ie. the impact of violating the boundary conditions in each case is different.)
#TODO: choose better testing parameters to lower this
SrcList = ['RawVec', 'MagDipole_Bfield', 'MagDipole', 'CircularLoop']
class FDEM_CrossCheck(unittest.TestCase):
if testBH:
def test_BH_CrossCheck_jxr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jxr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jyr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jyr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jzr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jzr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jxi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jxi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jyi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jyi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jzi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jzi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_exr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'exr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_eyr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'eyr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_ezr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'ezr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_exi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'exi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_eyi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'eyi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_ezi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'ezi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bxr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bxr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_byr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'byr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bzr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bzr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bxi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bxi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_byi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'byi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bzi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bzi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hxr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hxr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hyr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hyr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hzr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hzr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hxi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hxi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hyi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hyi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hzi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hzi', verbose=verbose, TOL=TOLEJHB))
if testBH:
def test_BH_CrossCheck_jxr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jxr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jyr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jyr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jzr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jzr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jxi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jxi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jyi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jyi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_jzi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'jzi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_exr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'exr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_eyr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'eyr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_ezr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'ezr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_exi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'exi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_eyi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'eyi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_ezi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'ezi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bxr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bxr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_byr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'byr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bzr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bzr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bxi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bxi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_byi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'byi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_bzi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'bzi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hxr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hxr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hyr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hyr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hzr(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hzr', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hxi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hxi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hyi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hyi', verbose=verbose, TOL=TOLEJHB))
def test_BH_CrossCheck_hzi(self):
self.assertTrue(crossCheckTest(SrcList, 'b', 'h', 'hzi', verbose=verbose, TOL=TOLEJHB))
if __name__ == '__main__':
unittest.main()
@@ -5,8 +5,8 @@ import sys
from scipy.constants import mu_0
from SimPEG.EM.Utils.testingUtils import getFDEMProblem
testEB = True
testHJ = True
testE = True
testB = True
verbose = False
@@ -17,10 +17,10 @@ MU = mu_0
freq = 1e-1
addrandoms = True
SrcType = 'RawVec' #or 'MAgDipole_Bfield', 'CircularLoop', 'RawVec'
SrcList = ['RawVec', 'MagDipole'] #or 'MAgDipole_Bfield', 'CircularLoop', 'RawVec'
def adjointTest(fdemType, comp):
prb = getFDEMProblem(fdemType, comp, [SrcType], freq)
prb = getFDEMProblem(fdemType, comp, SrcList, freq)
print 'Adjoint %s formulation - %s' % (fdemType, comp)
m = np.log(np.ones(prb.mapping.nP)*CONDUCTIVITY)
@@ -45,7 +45,7 @@ def adjointTest(fdemType, comp):
return np.abs(vJw - wJtv) < tol
class FDEM_AdjointTests(unittest.TestCase):
if testEB:
if testE:
def test_Jtvec_adjointTest_exr_Eform(self):
self.assertTrue(adjointTest('e', 'exr'))
def test_Jtvec_adjointTest_eyr_Eform(self):
@@ -72,6 +72,33 @@ class FDEM_AdjointTests(unittest.TestCase):
def test_Jtvec_adjointTest_bzi_Eform(self):
self.assertTrue(adjointTest('e', 'bzi'))
def test_Jtvec_adjointTest_jxr_Eform(self):
self.assertTrue(adjointTest('e', 'jxr'))
def test_Jtvec_adjointTest_jyr_Eform(self):
self.assertTrue(adjointTest('e', 'jyr'))
def test_Jtvec_adjointTest_jzr_Eform(self):
self.assertTrue(adjointTest('e', 'jzr'))
def test_Jtvec_adjointTest_jxi_Eform(self):
self.assertTrue(adjointTest('e', 'jxi'))
def test_Jtvec_adjointTest_jyi_Eform(self):
self.assertTrue(adjointTest('e', 'jyi'))
def test_Jtvec_adjointTest_jzi_Eform(self):
self.assertTrue(adjointTest('e', 'jzi'))
def test_Jtvec_adjointTest_hxr_Eform(self):
self.assertTrue(adjointTest('e', 'hxr'))
def test_Jtvec_adjointTest_hyr_Eform(self):
self.assertTrue(adjointTest('e', 'hyr'))
def test_Jtvec_adjointTest_hzr_Eform(self):
self.assertTrue(adjointTest('e', 'hzr'))
def test_Jtvec_adjointTest_hxi_Eform(self):
self.assertTrue(adjointTest('e', 'hxi'))
def test_Jtvec_adjointTest_hyi_Eform(self):
self.assertTrue(adjointTest('e', 'hyi'))
def test_Jtvec_adjointTest_hzi_Eform(self):
self.assertTrue(adjointTest('e', 'hzi'))
if testB:
def test_Jtvec_adjointTest_exr_Bform(self):
self.assertTrue(adjointTest('b', 'exr'))
def test_Jtvec_adjointTest_eyr_Bform(self):
@@ -84,6 +111,7 @@ class FDEM_AdjointTests(unittest.TestCase):
self.assertTrue(adjointTest('b', 'eyi'))
def test_Jtvec_adjointTest_ezi_Bform(self):
self.assertTrue(adjointTest('b', 'ezi'))
def test_Jtvec_adjointTest_bxr_Bform(self):
self.assertTrue(adjointTest('b', 'bxr'))
def test_Jtvec_adjointTest_byr_Bform(self):
@@ -97,59 +125,31 @@ class FDEM_AdjointTests(unittest.TestCase):
def test_Jtvec_adjointTest_bzi_Bform(self):
self.assertTrue(adjointTest('b', 'bzi'))
def test_Jtvec_adjointTest_jxr_Bform(self):
self.assertTrue(adjointTest('b', 'jxr'))
def test_Jtvec_adjointTest_jyr_Bform(self):
self.assertTrue(adjointTest('b', 'jyr'))
def test_Jtvec_adjointTest_jzr_Bform(self):
self.assertTrue(adjointTest('b', 'jzr'))
def test_Jtvec_adjointTest_jxi_Bform(self):
self.assertTrue(adjointTest('b', 'jxi'))
def test_Jtvec_adjointTest_jyi_Bform(self):
self.assertTrue(adjointTest('b', 'jyi'))
def test_Jtvec_adjointTest_jzi_Bform(self):
self.assertTrue(adjointTest('b', 'jzi'))
if testHJ:
def test_Jtvec_adjointTest_jxr_Jform(self):
self.assertTrue(adjointTest('j', 'jxr'))
def test_Jtvec_adjointTest_jyr_Jform(self):
self.assertTrue(adjointTest('j', 'jyr'))
def test_Jtvec_adjointTest_jzr_Jform(self):
self.assertTrue(adjointTest('j', 'jzr'))
def test_Jtvec_adjointTest_jxi_Jform(self):
self.assertTrue(adjointTest('j', 'jxi'))
def test_Jtvec_adjointTest_jyi_Jform(self):
self.assertTrue(adjointTest('j', 'jyi'))
def test_Jtvec_adjointTest_jzi_Jform(self):
self.assertTrue(adjointTest('j', 'jzi'))
def test_Jtvec_adjointTest_hxr_Jform(self):
self.assertTrue(adjointTest('j', 'hxr'))
def test_Jtvec_adjointTest_hyr_Jform(self):
self.assertTrue(adjointTest('j', 'hyr'))
def test_Jtvec_adjointTest_hzr_Jform(self):
self.assertTrue(adjointTest('j', 'hzr'))
def test_Jtvec_adjointTest_hxi_Jform(self):
self.assertTrue(adjointTest('j', 'hxi'))
def test_Jtvec_adjointTest_hyi_Jform(self):
self.assertTrue(adjointTest('j', 'hyi'))
def test_Jtvec_adjointTest_hzi_Jform(self):
self.assertTrue(adjointTest('j', 'hzi'))
def test_Jtvec_adjointTest_hxr_Hform(self):
self.assertTrue(adjointTest('h', 'hxr'))
def test_Jtvec_adjointTest_hyr_Hform(self):
self.assertTrue(adjointTest('h', 'hyr'))
def test_Jtvec_adjointTest_hzr_Hform(self):
self.assertTrue(adjointTest('h', 'hzr'))
def test_Jtvec_adjointTest_hxi_Hform(self):
self.assertTrue(adjointTest('h', 'hxi'))
def test_Jtvec_adjointTest_hyi_Hform(self):
self.assertTrue(adjointTest('h', 'hyi'))
def test_Jtvec_adjointTest_hzi_Hform(self):
self.assertTrue(adjointTest('h', 'hzi'))
def test_Jtvec_adjointTest_hxr_Hform(self):
self.assertTrue(adjointTest('h', 'jxr'))
def test_Jtvec_adjointTest_hyr_Hform(self):
self.assertTrue(adjointTest('h', 'jyr'))
def test_Jtvec_adjointTest_hzr_Hform(self):
self.assertTrue(adjointTest('h', 'jzr'))
def test_Jtvec_adjointTest_hxi_Hform(self):
self.assertTrue(adjointTest('h', 'jxi'))
def test_Jtvec_adjointTest_hyi_Hform(self):
self.assertTrue(adjointTest('h', 'jyi'))
def test_Jtvec_adjointTest_hzi_Hform(self):
self.assertTrue(adjointTest('h', 'jzi'))
def test_Jtvec_adjointTest_hxr_Bform(self):
self.assertTrue(adjointTest('b', 'hxr'))
def test_Jtvec_adjointTest_hyr_Bform(self):
self.assertTrue(adjointTest('b', 'hyr'))
def test_Jtvec_adjointTest_hzr_Bform(self):
self.assertTrue(adjointTest('b', 'hzr'))
def test_Jtvec_adjointTest_hxi_Bform(self):
self.assertTrue(adjointTest('b', 'hxi'))
def test_Jtvec_adjointTest_hyi_Bform(self):
self.assertTrue(adjointTest('b', 'hyi'))
def test_Jtvec_adjointTest_hzi_Bform(self):
self.assertTrue(adjointTest('b', 'hzi'))
if __name__ == '__main__':
@@ -0,0 +1,155 @@
import unittest
from SimPEG import *
from SimPEG import EM
import sys
from scipy.constants import mu_0
from SimPEG.EM.Utils.testingUtils import getFDEMProblem
testJ = True
testH = True
verbose = False
TOL = 1e-5
FLR = 1e-20 # "zero", so if residual below this --> pass regardless of order
CONDUCTIVITY = 1e1
MU = mu_0
freq = 1e-1
addrandoms = True
SrcList = ['RawVec', 'MagDipole'] #or 'MAgDipole_Bfield', 'CircularLoop', 'RawVec'
def adjointTest(fdemType, comp):
prb = getFDEMProblem(fdemType, comp, SrcList, freq)
print 'Adjoint %s formulation - %s' % (fdemType, comp)
m = np.log(np.ones(prb.mapping.nP)*CONDUCTIVITY)
mu = np.ones(prb.mesh.nC)*MU
if addrandoms is True:
m = m + np.random.randn(prb.mapping.nP)*np.log(CONDUCTIVITY)*1e-1
mu = mu + np.random.randn(prb.mesh.nC)*MU*1e-1
survey = prb.survey
u = prb.fields(m)
v = np.random.rand(survey.nD)
w = np.random.rand(prb.mesh.nC)
vJw = v.dot(prb.Jvec(m, w, u))
wJtv = w.dot(prb.Jtvec(m, v, u))
tol = np.max([TOL*(10**int(np.log10(np.abs(vJw)))),FLR])
print vJw, wJtv, vJw - wJtv, tol, np.abs(vJw - wJtv) < tol
return np.abs(vJw - wJtv) < tol
class FDEM_AdjointTests(unittest.TestCase):
if testJ:
def test_Jtvec_adjointTest_jxr_Jform(self):
self.assertTrue(adjointTest('j', 'jxr'))
def test_Jtvec_adjointTest_jyr_Jform(self):
self.assertTrue(adjointTest('j', 'jyr'))
def test_Jtvec_adjointTest_jzr_Jform(self):
self.assertTrue(adjointTest('j', 'jzr'))
def test_Jtvec_adjointTest_jxi_Jform(self):
self.assertTrue(adjointTest('j', 'jxi'))
def test_Jtvec_adjointTest_jyi_Jform(self):
self.assertTrue(adjointTest('j', 'jyi'))
def test_Jtvec_adjointTest_jzi_Jform(self):
self.assertTrue(adjointTest('j', 'jzi'))
def test_Jtvec_adjointTest_hxr_Jform(self):
self.assertTrue(adjointTest('j', 'hxr'))
def test_Jtvec_adjointTest_hyr_Jform(self):
self.assertTrue(adjointTest('j', 'hyr'))
def test_Jtvec_adjointTest_hzr_Jform(self):
self.assertTrue(adjointTest('j', 'hzr'))
def test_Jtvec_adjointTest_hxi_Jform(self):
self.assertTrue(adjointTest('j', 'hxi'))
def test_Jtvec_adjointTest_hyi_Jform(self):
self.assertTrue(adjointTest('j', 'hyi'))
def test_Jtvec_adjointTest_hzi_Jform(self):
self.assertTrue(adjointTest('j', 'hzi'))
def test_Jtvec_adjointTest_exr_Jform(self):
self.assertTrue(adjointTest('j', 'exr'))
def test_Jtvec_adjointTest_eyr_Jform(self):
self.assertTrue(adjointTest('j', 'eyr'))
def test_Jtvec_adjointTest_ezr_Jform(self):
self.assertTrue(adjointTest('j', 'ezr'))
def test_Jtvec_adjointTest_exi_Jform(self):
self.assertTrue(adjointTest('j', 'exi'))
def test_Jtvec_adjointTest_eyi_Jform(self):
self.assertTrue(adjointTest('j', 'eyi'))
def test_Jtvec_adjointTest_ezi_Jform(self):
self.assertTrue(adjointTest('j', 'ezi'))
def test_Jtvec_adjointTest_bxr_Jform(self):
self.assertTrue(adjointTest('j', 'bxr'))
def test_Jtvec_adjointTest_byr_Jform(self):
self.assertTrue(adjointTest('j', 'byr'))
def test_Jtvec_adjointTest_bzr_Jform(self):
self.assertTrue(adjointTest('j', 'bzr'))
def test_Jtvec_adjointTest_bxi_Jform(self):
self.assertTrue(adjointTest('j', 'bxi'))
def test_Jtvec_adjointTest_byi_Jform(self):
self.assertTrue(adjointTest('j', 'byi'))
def test_Jtvec_adjointTest_bzi_Jform(self):
self.assertTrue(adjointTest('j', 'bzi'))
if testH:
def test_Jtvec_adjointTest_hxr_Hform(self):
self.assertTrue(adjointTest('h', 'hxr'))
def test_Jtvec_adjointTest_hyr_Hform(self):
self.assertTrue(adjointTest('h', 'hyr'))
def test_Jtvec_adjointTest_hzr_Hform(self):
self.assertTrue(adjointTest('h', 'hzr'))
def test_Jtvec_adjointTest_hxi_Hform(self):
self.assertTrue(adjointTest('h', 'hxi'))
def test_Jtvec_adjointTest_hyi_Hform(self):
self.assertTrue(adjointTest('h', 'hyi'))
def test_Jtvec_adjointTest_hzi_Hform(self):
self.assertTrue(adjointTest('h', 'hzi'))
def test_Jtvec_adjointTest_jxr_Hform(self):
self.assertTrue(adjointTest('h', 'jxr'))
def test_Jtvec_adjointTest_jyr_Hform(self):
self.assertTrue(adjointTest('h', 'jyr'))
def test_Jtvec_adjointTest_jzr_Hform(self):
self.assertTrue(adjointTest('h', 'jzr'))
def test_Jtvec_adjointTest_jxi_Hform(self):
self.assertTrue(adjointTest('h', 'jxi'))
def test_Jtvec_adjointTest_jyi_Hform(self):
self.assertTrue(adjointTest('h', 'jyi'))
def test_Jtvec_adjointTest_jzi_Hform(self):
self.assertTrue(adjointTest('h', 'jzi'))
def test_Jtvec_adjointTest_exr_Hform(self):
self.assertTrue(adjointTest('h', 'exr'))
def test_Jtvec_adjointTest_eyr_Hform(self):
self.assertTrue(adjointTest('h', 'eyr'))
def test_Jtvec_adjointTest_ezr_Hform(self):
self.assertTrue(adjointTest('h', 'ezr'))
def test_Jtvec_adjointTest_exi_Hform(self):
self.assertTrue(adjointTest('h', 'exi'))
def test_Jtvec_adjointTest_eyi_Hform(self):
self.assertTrue(adjointTest('h', 'eyi'))
def test_Jtvec_adjointTest_ezi_Hform(self):
self.assertTrue(adjointTest('h', 'ezi'))
def test_Jtvec_adjointTest_bxr_Hform(self):
self.assertTrue(adjointTest('h', 'bxr'))
def test_Jtvec_adjointTest_byr_Hform(self):
self.assertTrue(adjointTest('h', 'byr'))
def test_Jtvec_adjointTest_bzr_Hform(self):
self.assertTrue(adjointTest('h', 'bzr'))
def test_Jtvec_adjointTest_bxi_Hform(self):
self.assertTrue(adjointTest('h', 'bxi'))
def test_Jtvec_adjointTest_byi_Hform(self):
self.assertTrue(adjointTest('h', 'byi'))
def test_Jtvec_adjointTest_bzi_Hform(self):
self.assertTrue(adjointTest('h', 'bzi'))
if __name__ == '__main__':
unittest.main()
+116 -10
View File
@@ -5,9 +5,11 @@ import sys
from scipy.constants import mu_0
from SimPEG.EM.Utils.testingUtils import getFDEMProblem
testDerivs = True
testEB = True
testHJ = True
testE = True
testB = True
testH = True
testJ = True
verbose = False
@@ -18,12 +20,12 @@ MU = mu_0
freq = 1e-1
addrandoms = True
SrcType = 'RawVec' #or 'MAgDipole_Bfield', 'CircularLoop', 'RawVec'
SrcType = ['MagDipole', 'RawVec'] #or 'MAgDipole_Bfield', 'CircularLoop', 'RawVec'
def derivTest(fdemType, comp):
prb = getFDEMProblem(fdemType, comp, [SrcType], freq)
prb = getFDEMProblem(fdemType, comp, SrcType, freq)
print '%s formulation - %s' % (fdemType, comp)
x0 = np.log(np.ones(prb.mapping.nP)*CONDUCTIVITY)
mu = np.log(np.ones(prb.mesh.nC)*MU)
@@ -32,9 +34,6 @@ def derivTest(fdemType, comp):
x0 = x0 + np.random.randn(prb.mapping.nP)*np.log(CONDUCTIVITY)*1e-1
mu = mu + np.random.randn(prb.mapping.nP)*MU*1e-1
# prb.PropMap.PropModel.mu = mu
# prb.PropMap.PropModel.mui = 1./mu
survey = prb.survey
def fun(x):
return survey.dpred(x), lambda x: prb.Jvec(x0, x)
@@ -43,7 +42,7 @@ def derivTest(fdemType, comp):
class FDEM_DerivTests(unittest.TestCase):
if testEB:
if testE:
def test_Jvec_exr_Eform(self):
self.assertTrue(derivTest('e', 'exr'))
def test_Jvec_eyr_Eform(self):
@@ -70,6 +69,33 @@ class FDEM_DerivTests(unittest.TestCase):
def test_Jvec_bzi_Eform(self):
self.assertTrue(derivTest('e', 'bzi'))
def test_Jvec_exr_Eform(self):
self.assertTrue(derivTest('e', 'jxr'))
def test_Jvec_eyr_Eform(self):
self.assertTrue(derivTest('e', 'jyr'))
def test_Jvec_ezr_Eform(self):
self.assertTrue(derivTest('e', 'jzr'))
def test_Jvec_exi_Eform(self):
self.assertTrue(derivTest('e', 'jxi'))
def test_Jvec_eyi_Eform(self):
self.assertTrue(derivTest('e', 'jyi'))
def test_Jvec_ezi_Eform(self):
self.assertTrue(derivTest('e', 'jzi'))
def test_Jvec_bxr_Eform(self):
self.assertTrue(derivTest('e', 'hxr'))
def test_Jvec_byr_Eform(self):
self.assertTrue(derivTest('e', 'hyr'))
def test_Jvec_bzr_Eform(self):
self.assertTrue(derivTest('e', 'hzr'))
def test_Jvec_bxi_Eform(self):
self.assertTrue(derivTest('e', 'hxi'))
def test_Jvec_byi_Eform(self):
self.assertTrue(derivTest('e', 'hyi'))
def test_Jvec_bzi_Eform(self):
self.assertTrue(derivTest('e', 'hzi'))
if testB:
def test_Jvec_exr_Bform(self):
self.assertTrue(derivTest('b', 'exr'))
def test_Jvec_eyr_Bform(self):
@@ -96,7 +122,33 @@ class FDEM_DerivTests(unittest.TestCase):
def test_Jvec_bzi_Bform(self):
self.assertTrue(derivTest('b', 'bzi'))
if testHJ:
def test_Jvec_jxr_Bform(self):
self.assertTrue(derivTest('b', 'jxr'))
def test_Jvec_jyr_Bform(self):
self.assertTrue(derivTest('b', 'jyr'))
def test_Jvec_jzr_Bform(self):
self.assertTrue(derivTest('b', 'jzr'))
def test_Jvec_jxi_Bform(self):
self.assertTrue(derivTest('b', 'jxi'))
def test_Jvec_jyi_Bform(self):
self.assertTrue(derivTest('b', 'jyi'))
def test_Jvec_jzi_Bform(self):
self.assertTrue(derivTest('b', 'jzi'))
def test_Jvec_hxr_Bform(self):
self.assertTrue(derivTest('b', 'hxr'))
def test_Jvec_hyr_Bform(self):
self.assertTrue(derivTest('b', 'hyr'))
def test_Jvec_hzr_Bform(self):
self.assertTrue(derivTest('b', 'hzr'))
def test_Jvec_hxi_Bform(self):
self.assertTrue(derivTest('b', 'hxi'))
def test_Jvec_hyi_Bform(self):
self.assertTrue(derivTest('b', 'hyi'))
def test_Jvec_hzi_Bform(self):
self.assertTrue(derivTest('b', 'hzi'))
if testJ:
def test_Jvec_jxr_Jform(self):
self.assertTrue(derivTest('j', 'jxr'))
def test_Jvec_jyr_Jform(self):
@@ -123,6 +175,34 @@ class FDEM_DerivTests(unittest.TestCase):
def test_Jvec_hzi_Jform(self):
self.assertTrue(derivTest('j', 'hzi'))
def test_Jvec_exr_Jform(self):
self.assertTrue(derivTest('j', 'exr'))
def test_Jvec_eyr_Jform(self):
self.assertTrue(derivTest('j', 'eyr'))
def test_Jvec_ezr_Jform(self):
self.assertTrue(derivTest('j', 'ezr'))
def test_Jvec_exi_Jform(self):
self.assertTrue(derivTest('j', 'exi'))
def test_Jvec_eyi_Jform(self):
self.assertTrue(derivTest('j', 'eyi'))
def test_Jvec_ezi_Jform(self):
self.assertTrue(derivTest('j', 'ezi'))
def test_Jvec_bxr_Jform(self):
self.assertTrue(derivTest('j', 'bxr'))
def test_Jvec_byr_Jform(self):
self.assertTrue(derivTest('j', 'byr'))
def test_Jvec_bzr_Jform(self):
self.assertTrue(derivTest('j', 'bzr'))
def test_Jvec_bxi_Jform(self):
self.assertTrue(derivTest('j', 'bxi'))
def test_Jvec_byi_Jform(self):
self.assertTrue(derivTest('j', 'byi'))
def test_Jvec_bzi_Jform(self):
self.assertTrue(derivTest('j', 'bzi'))
if testH:
def test_Jvec_hxr_Hform(self):
self.assertTrue(derivTest('h', 'hxr'))
def test_Jvec_hyr_Hform(self):
@@ -149,6 +229,32 @@ class FDEM_DerivTests(unittest.TestCase):
def test_Jvec_hzi_Hform(self):
self.assertTrue(derivTest('h', 'jzi'))
def test_Jvec_exr_Hform(self):
self.assertTrue(derivTest('h', 'exr'))
def test_Jvec_eyr_Hform(self):
self.assertTrue(derivTest('h', 'eyr'))
def test_Jvec_ezr_Hform(self):
self.assertTrue(derivTest('h', 'ezr'))
def test_Jvec_exi_Hform(self):
self.assertTrue(derivTest('h', 'exi'))
def test_Jvec_eyi_Hform(self):
self.assertTrue(derivTest('h', 'eyi'))
def test_Jvec_ezi_Hform(self):
self.assertTrue(derivTest('h', 'ezi'))
def test_Jvec_bxr_Hform(self):
self.assertTrue(derivTest('h', 'bxr'))
def test_Jvec_byr_Hform(self):
self.assertTrue(derivTest('h', 'byr'))
def test_Jvec_bzr_Hform(self):
self.assertTrue(derivTest('h', 'bzr'))
def test_Jvec_bxi_Hform(self):
self.assertTrue(derivTest('h', 'bxi'))
def test_Jvec_byi_Hform(self):
self.assertTrue(derivTest('h', 'byi'))
def test_Jvec_bzi_Hform(self):
self.assertTrue(derivTest('h', 'bzi'))
if __name__ == '__main__':
unittest.main()
+3 -1
View File
@@ -10,7 +10,9 @@ except ImportError, e:
MumpsSolver = SolverLU
def halfSpaceProblemAnaDiff(meshType, sig_half=1e-2, rxOffset=50., bounds=[1e-5,1e-3], showIt=False):
def halfSpaceProblemAnaDiff(meshType, sig_half=1e-2, rxOffset=50., bounds=None, showIt=False):
if bounds is None:
bounds = [1e-5,1e-3]
if meshType == 'CYL':
cs, ncx, ncz, npad = 5., 30, 10, 15
hx = [(cs,ncx), (cs,npad,1.3)]
+6 -6
View File
@@ -116,8 +116,8 @@ class RichardsTests1D(unittest.TestCase):
v = np.random.rand(self.survey.nD)
z = np.random.rand(self.M.nC)
Hs = self.prob.fields(self.Ks)
vJz = v.dot(self.prob.Jvec(self.Ks,z,u=Hs))
zJv = z.dot(self.prob.Jtvec(self.Ks,v,u=Hs))
vJz = v.dot(self.prob.Jvec(self.Ks,z,f=Hs))
zJv = z.dot(self.prob.Jtvec(self.Ks,v,f=Hs))
tol = TOL*(10**int(np.log10(np.abs(zJv))))
passed = np.abs(vJz - zJv) < tol
print 'Richards Adjoint Test - PressureHead'
@@ -188,8 +188,8 @@ class RichardsTests2D(unittest.TestCase):
v = np.random.rand(self.survey.nD)
z = np.random.rand(self.M.nC)
Hs = self.prob.fields(self.Ks)
vJz = v.dot(self.prob.Jvec(self.Ks,z,u=Hs))
zJv = z.dot(self.prob.Jtvec(self.Ks,v,u=Hs))
vJz = v.dot(self.prob.Jvec(self.Ks,z,f=Hs))
zJv = z.dot(self.prob.Jtvec(self.Ks,v,f=Hs))
tol = TOL*(10**int(np.log10(np.abs(zJv))))
passed = np.abs(vJz - zJv) < tol
print '2D: Richards Adjoint Test - PressureHead'
@@ -260,8 +260,8 @@ class RichardsTests3D(unittest.TestCase):
v = np.random.rand(self.survey.nD)
z = np.random.rand(self.M.nC)
Hs = self.prob.fields(self.Ks)
vJz = v.dot(self.prob.Jvec(self.Ks,z,u=Hs))
zJv = z.dot(self.prob.Jtvec(self.Ks,v,u=Hs))
vJz = v.dot(self.prob.Jvec(self.Ks,z,f=Hs))
zJv = z.dot(self.prob.Jtvec(self.Ks,v,f=Hs))
tol = TOL*(10**int(np.log10(np.abs(zJv))))
passed = np.abs(vJz - zJv) < tol
print '3D: Richards Adjoint Test - PressureHead'
+80 -4
View File
@@ -146,6 +146,20 @@ class TestCyl2DMesh(unittest.TestCase):
assert np.abs(Pr*(Pc2r*mc) - Pc*mc).max() < 1e-3
def test_getInterpMatCartMesh_Cells2Nodes(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
Mc = Mesh.CylMesh([np.ones(10)/5,1,10],x0='0C0',cartesianOrigin=[-0.2,-0.2,0])
mc = np.arange(Mc.nC)
xr = np.linspace(0,0.4,50)
xc = np.linspace(0,0.4,50) + 0.2
Pr = Mr.getInterpolationMat(np.c_[xr,np.ones(50)*-0.2,np.ones(50)*0.5],'N')
Pc = Mc.getInterpolationMat(np.c_[xc,np.zeros(50),np.ones(50)*0.5],'CC')
Pc2r = Mc.getInterpolationMatCartMesh(Mr, 'CC', locTypeTo='N')
assert np.abs(Pr*(Pc2r*mc) - Pc*mc).max() < 1e-3
def test_getInterpMatCartMesh_Faces(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
@@ -177,6 +191,37 @@ class TestCyl2DMesh(unittest.TestCase):
assert np.abs(mag[dist > 0.1].min() - 1) < TOL
def test_getInterpMatCartMesh_Faces2Edges(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
Mc = Mesh.CylMesh([np.ones(10)/5,1,10],x0='0C0',cartesianOrigin=[-0.2,-0.2,0])
Pf2e = Mc.getInterpolationMatCartMesh(Mr, 'F', locTypeTo='E')
mf = np.ones(Mc.nF)
ecart = Pf2e * mf
excc = Mr.aveEx2CC*Mr.r(ecart, 'E', 'Ex')
eycc = Mr.aveEy2CC*Mr.r(ecart, 'E', 'Ey')
ezcc = Mr.r(ecart, 'E', 'Ez')
indX = Utils.closestPoints(Mr, [0.45, -0.2, 0.5])
indY = Utils.closestPoints(Mr, [-0.2, 0.45, 0.5])
TOL = 1e-2
assert np.abs(float(excc[indX]) - 1) < TOL
assert np.abs(float(excc[indY]) - 0) < TOL
assert np.abs(float(eycc[indX]) - 0) < TOL
assert np.abs(float(eycc[indY]) - 1) < TOL
assert np.abs((ezcc - 1).sum()) < TOL
mag = (excc**2 + eycc**2)**0.5
dist = ((Mr.gridCC[:,0] + 0.2)**2 + (Mr.gridCC[:,1] + 0.2)**2)**0.5
assert np.abs(mag[dist > 0.1].max() - 1) < TOL
assert np.abs(mag[dist > 0.1].min() - 1) < TOL
def test_getInterpMatCartMesh_Edges(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
@@ -185,11 +230,42 @@ class TestCyl2DMesh(unittest.TestCase):
Pe = Mc.getInterpolationMatCartMesh(Mr, 'E')
me = np.ones(Mc.nE)
erect = Pe * me
ecart = Pe * me
excc = Mr.aveEx2CC*Mr.r(erect, 'E', 'Ex')
eycc = Mr.aveEy2CC*Mr.r(erect, 'E', 'Ey')
ezcc = Mr.r(erect, 'E', 'Ez')
excc = Mr.aveEx2CC*Mr.r(ecart, 'E', 'Ex')
eycc = Mr.aveEy2CC*Mr.r(ecart, 'E', 'Ey')
ezcc = Mr.aveEz2CC*Mr.r(ecart, 'E', 'Ez')
indX = Utils.closestPoints(Mr, [0.45, -0.2, 0.5])
indY = Utils.closestPoints(Mr, [-0.2, 0.45, 0.5])
TOL = 1e-2
assert np.abs(float(excc[indX]) - 0) < TOL
assert np.abs(float(excc[indY]) + 1) < TOL
assert np.abs(float(eycc[indX]) - 1) < TOL
assert np.abs(float(eycc[indY]) - 0) < TOL
assert np.abs(ezcc.sum()) < TOL
mag = (excc**2 + eycc**2)**0.5
dist = ((Mr.gridCC[:,0] + 0.2)**2 + (Mr.gridCC[:,1] + 0.2)**2)**0.5
assert np.abs(mag[dist > 0.1].max() - 1) < TOL
assert np.abs(mag[dist > 0.1].min() - 1) < TOL
def test_getInterpMatCartMesh_Edges2Faces(self):
Mr = Mesh.TensorMesh([100,100,2], x0='CC0')
Mc = Mesh.CylMesh([np.ones(10)/5,1,10],x0='0C0',cartesianOrigin=[-0.2,-0.2,0])
Pe2f = Mc.getInterpolationMatCartMesh(Mr, 'E', locTypeTo='F')
me = np.ones(Mc.nE)
frect = Pe2f * me
excc = Mr.aveFx2CC*Mr.r(frect, 'F', 'Fx')
eycc = Mr.aveFy2CC*Mr.r(frect, 'F', 'Fy')
ezcc = Mr.r(frect, 'F', 'Fz')
indX = Utils.closestPoints(Mr, [0.45, -0.2, 0.5])
indY = Utils.closestPoints(Mr, [-0.2, 0.45, 0.5])
@@ -242,9 +242,6 @@ class TestAnalytics(unittest.TestCase):
def test_appRes1en3(self):self.assertTrue(appResPhsHalfspace_eFrom_ps_Norm(1e-3))
def test_appPhs1en3(self):self.assertTrue(appResPhsHalfspace_eFrom_ps_Norm(1e-3,False))
# Do a derivative test
def test_derivProj1(self):self.assertTrue(DerivProjfieldsTest(halfSpace(1e-2)))
# Do a derivative test of Jvec
# def test_derivJvec_zxxr(self):self.assertTrue(DerivJvecTest(random(1e-2),'zxxr',.1))
# def test_derivJvec_zxxi(self):self.assertTrue(DerivJvecTest(random(1e-2),'zxxi',.1))