Files
simpeg/simpegMT/ProblemMT.py
T
Gudni Karl Rosenkjaer 52618bac35 Fixed bugs. Added notebooks with halfspace and layer examples.
Code is working (returning results with in couple of % for a 1D analytic solution) but test need to be "automated".
2015-03-02 14:58:53 -08:00

282 lines
8.8 KiB
Python

from SimPEG import Survey, Problem, Utils, Models, np, sp, SolverLU as SimpegSolver
from scipy.constants import mu_0
from SurveyMT import SurveyMT, FieldsMT
def omega(freq):
"""Change frequency to angular frequency, omega"""
return 2.*np.pi*freq
class MTProblem(Problem.BaseProblem):
def __init__(self, mesh, **kwargs):
Problem.BaseProblem.__init__(self, mesh, **kwargs)
solType = 'e'
storeTheseFields = ['e', 'b']
surveyPair = SurveyMT
dataPair = Survey.Data
Solver = SimpegSolver
solverOpts = {}
####################################################
# Mass Matrices
####################################################
@property
def MfMui(self):
#TODO: assuming constant mu
if getattr(self, '_MfMui', None) is None:
self._MfMui = self.mesh.getFaceInnerProduct(1/mu_0)
return self._MfMui
@property
def Me(self):
if getattr(self, '_Me', None) is None:
self._Me = self.mesh.getEdgeInnerProduct()
return self._Me
@property
def MeSigma(self):
#TODO: hardcoded to sigma as the model
if getattr(self, '_MeSigma', None) is None:
sigma = self.curTModel
self._MeSigma = self.mesh.getEdgeInnerProduct(sigma)
return self._MeSigma
@property
def MeSigmaI(self):
#TODO: hardcoded to sigma as the model
if getattr(self, '_MeSigmaI', None) is None:
sigma = self.curTModel
self._MeSigmaI = self.mesh.getEdgeInnerProduct(sigma, invMat=True)
return self._MeSigmaI
curModel = Utils.dependentProperty('_curModel', None, ['_MeSigma', '_MeSigmaI', '_curTModel', '_curTModelDeriv'], 'Sets the current model, and removes dependent mass matrices.')
@property
def curTModel(self):
if getattr(self, '_curTModel', None) is None:
self._curTModel = self.mapping*self.curModel
return self._curTModel
@property
def curTModelDeriv(self):
if getattr(self, '_curTModelDeriv', None) is None:
self._curTModelDeriv = self.mapping*self.curModel
return self._curTModelDeriv
# Background model
@property
def backModel(self):
"""
Sets the model, and removes dependent mass matrices.
"""
return getattr(self, '_backModel', None)
@backModel.setter
def backModel(self, value):
if value is self.backModel:
return # it is the same!
self._backModel = Models.Model(value, self.mapping)
for prop in self.deleteTheseOnModelUpdate:
if hasattr(self, prop):
delattr(self, prop)
@property
def MeSigmaBG(self):
#TODO: hardcoded to sigma as the model
if getattr(self, '_MeSigmaBG', None) is None:
sigmaBG = self.backModel
self._MeSigmaBG = self.mesh.getEdgeInnerProduct(sigmaBG)
return self._MeSigmaBG
def fields(self, m, m_back):
'''
Function to calculate all the fields for the model m.
:param np.ndarray (nC,) m: Conductivity model
:param np.ndarray (nC,) m_back: Background conductivity model
'''
self.curModel = m
self.backModel = m_back
# RHS, CalcFields = self.getRHS(freq,m_back), self.calcFields
F = FieldsMT(self.mesh, self.survey)
#NOTE: add print status statements.
for freq in self.survey.freqs:
A = self.getA(freq)
rhs = self.getRHS(freq,m_back)
Ainv = self.Solver(A, **self.solverOpts)
e = Ainv * rhs
# Store the fields
Src = self.survey.getSources(freq)
# Store the fields
F[Src, 'e_px'] = e[:,0]
F[Src, 'e_py'] = e[:,1]
# Note curl e = -iwb so b = -curl/iw
b = -( self.mesh.edgeCurl * e )/( 1j*omega(freq) )
F[Src, 'b_px'] = b[:,0]
F[Src, 'b_py'] = b[:,1]
return F
def getA(self, freq):
"""
Function to get the A matrix.
:param float freq: Frequency
:rtype: scipy.sparse.csr_matrix
:return: A
"""
mui = self.MfMui
sig = self.MeSigma
C = self.mesh.edgeCurl
return C.T*mui*C - 1j*omega(freq)*sig
def getAbg(self, freq):
"""
Function to get the A matrix for the background model.
:param float freq: Frequency
:rtype: scipy.sparse.csr_matrix
:return: A
"""
mui = self.MfMui
sigBG = self.MeSigmaBG
C = self.mesh.edgeCurl
return C.T*mui*C - 1j*omega(freq)*sigBG
def getADeriv(self, freq, u, v, adjoint=False):
sig = self.curTModel
dsig_dm = self.curTModelDeriv
dMe_dsig = self.mesh.getEdgeInnerProductDeriv(sig, v=u)
if adjoint:
return 1j * omega(freq) * ( dsig_dm.T * ( dMe_dsig.T * v ) )
return 1j * omega(freq) * ( dMe_dsig * ( dsig_dm * v ) )
def getRHS(self, freq, backSigma):
"""
Function to return the right hand side for the system.
:param float freq: Frequency
:param numpy.ndarray (nC,) backSigma: Background conductivity model
:rtype: numpy.ndarray (nE, 2)
:return: one RHS for both polarizations
"""
# Get sources for the frequency
src = self.survey.getSources(freq)
# Make sure that there is 2 polarizations.
# assert len()
# Get the background electric fields
from simpegMT.Sources import homo1DModelSource
eBG_bp = homo1DModelSource(self.mesh,freq,backSigma)
Abg = self.getAbg(freq)
return -Abg*eBG_bp
##################################################################
# Inversion stuff
##################################################################
# Not really used now....
def calcFields(self, sol, freq, fieldType, adjoint=False):
e = sol
if fieldType == 'e':
return e
elif fieldType == 'b':
if not adjoint:
b = -(1./(1j*omega(freq))) * ( self.mesh.edgeCurl * e )
else:
b = -(1./(1j*omega(freq))) * ( self.mesh.edgeCurl.T * e )
return b
raise NotImplementedError('fieldType "%s" is not implemented.' % fieldType)
def calcFieldsDeriv(self, sol, freq, fieldType, v, adjoint=False):
e = sol
if fieldType == 'e':
return None
elif fieldType == 'b':
return None
raise NotImplementedError('fieldType "%s" is not implemented.' % fieldType)
def Jvec(self, m, v, u=None):
if u is None:
u = self.fields(m)
self.curModel = m
Jv = self.dataPair(self.survey)
for freq in self.survey.freqs:
A = self.getA(freq)
solver = self.Solver(A, **self.solverOpts)
for tx in self.survey.getTransmitters(freq):
u_tx = u[tx, self.solType]
w = self.getADeriv(freq, u_tx, v)
Ainvw = solver.solve(w)
for rx in tx.rxList:
fAinvw = self.calcFields(Ainvw, freq, rx.projField)
P = lambda v: rx.projectFieldsDeriv(tx, self.mesh, u, v)
df_dm = self.calcFieldsDeriv(u_tx, freq, rx.projField, v)
if df_dm is None:
Jv[tx, rx] = - P(fAinvw)
else:
Jv[tx, rx] = - P(fAinvw) + P(df_dm)
return Utils.mkvc(Jv)
def Jtvec(self, m, v, u=None):
if u is None:
u = self.fields(m)
self.curModel = m
# Ensure v is a data object.
if not isinstance(v, self.dataPair):
v = self.dataPair(self.survey, v)
Jtv = np.zeros(self.mapping.nP)
for freq in self.survey.freqs:
AT = self.getA(freq).T
solver = self.Solver(AT, **self.solverOpts)
for tx in self.survey.getTransmitters(freq):
u_tx = u[tx, self.solType]
for rx in tx.rxList:
PTv = rx.projectFieldsDeriv(tx, self.mesh, u, v[tx, rx], adjoint=True)
fPTv = self.calcFields(PTv, freq, rx.projField, adjoint=True)
w = solver.solve( fPTv )
Jtv_rx = - self.getADeriv(freq, u_tx, w, adjoint=True)
df_dm = self.calcFieldsDeriv(u_tx, freq, rx.projField, PTv, adjoint=True)
if df_dm is not None:
Jtv_rx += df_dm
real_or_imag = rx.projComp
if real_or_imag == 'real':
Jtv += Jtv_rx.real
elif real_or_imag == 'imag':
Jtv += - Jtv_rx.real
else:
raise Exception('Must be real or imag')
return Jtv