from SimPEG import Problem, Utils, np, sp, Solver as SimpegSolver from scipy.constants import mu_0 from SurveyFDEM import SurveyFDEM, DataFDEM, FieldsFDEM from simpegEM.Utils import Sources def omega(freq): """Change frequency to angular frequency, omega""" return 2.*np.pi*freq class BaseProblemFDEM(Problem.BaseProblem): """ Frequency-Domain EM problem - E-formulation .. math:: \dcurl E + i \omega B = 0 \\\\ \dcurl^\\top \MfMui B - \MeSig E = \Me \j_s """ def __init__(self, model, **kwargs): Problem.BaseProblem.__init__(self, model, **kwargs) storeTheseFields = ['e', 'b'] surveyPair = SurveyFDEM dataPair = DataFDEM 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.currentTransformedModel self._MeSigma = self.mesh.getEdgeInnerProduct(sigma) return self._MeSigma @property def MeSigmaI(self): # TODO: this will not work if tensor conductivity if getattr(self, '_MeSigmaI', None) is None: self._MeSigmaI = Utils.sdiag(1/self.MeSigma.diagonal()) return self._MeSigmaI currentTransformedModel = Utils.dependentProperty('_currentTransformedModel', None, ['_MeSigma', '_MeSigmaI'], 'Sets the current model, and removes dependent mass matrices.') def fields(self, m): self.currentTransformedModel = self.model.transform(m) F = self.forward(m, self.getRHS, self.calcFields) return F def forward(self, m, RHS, CalcFields): F = FieldsFDEM(self.mesh, self.survey) for freq in self.survey.freqs: A = self.getA(freq) rhs = RHS(freq) solver = self.Solver(A, **self.solverOpts) sol = solver.solve(rhs) F[freq] = CalcFields(sol, freq) return F class ProblemFDEM_e(BaseProblemFDEM): """ Solving for e! """ def __init__(self, model, **kwargs): BaseProblemFDEM.__init__(self, model, **kwargs) def getA(self, freq): """ :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 getRHS(self, freq): """ :param float freq: Frequency :rtype: numpy.ndarray (nE, nTx) :return: RHS """ Txs = self.survey.getTransmitters(freq) rhs = range(len(Txs)) for i, tx in enumerate(Txs): if tx.txType == 'VMD': src = Sources.MagneticDipoleVectorPotential else: raise NotImplemented('%s txType is not implemented' % tx.txType) SRCx = src(tx.loc, self.mesh.gridEx, 'x') SRCy = src(tx.loc, self.mesh.gridEy, 'y') SRCz = src(tx.loc, self.mesh.gridEz, 'z') rhs[i] = np.concatenate((SRCx, SRCy, SRCz)) a = np.concatenate(rhs).reshape((self.mesh.nE, len(Txs)), order='F') mui = self.MfMui C = self.mesh.edgeCurl j_s = C.T*mui*C*a return -1j*omega(freq)*j_s def calcFields(self, sol, freq): e = sol fDict = {} if 'e' in self.storeTheseFields: fDict['e'] = e if 'b' in self.storeTheseFields: b = -1./(1j*omega(freq))*self.mesh.edgeCurl*e fDict['b'] = b return fDict def Jvec(self, m, v, u=None): if u is None: u = self.fields(m) sig = self.model.transform(m) self.currentTransformedModel = sig Jv = self.dataPair(self.survey) dsig_dm = self.model.transformDeriv(m) for i, freq in enumerate(self.survey.freqs): e = u[freq, 'e'] A = self.getA(freq) solver = self.Solver(A, **self.solverOpts) for txi, tx in enumerate(self.survey.getTransmitters(freq)): dMe_dsig = self.mesh.getEdgeInnerProductDeriv(sig, v=e[:,txi]) P = tx.projectFieldsDeriv(self.mesh, u) b = 1j*omega(freq) * ( dMe_dsig * ( dsig_dm * v ) ) Ainvb = solver.solve(b) Jv[tx] = -P*Ainvb return Utils.mkvc(Jv) def Jtvec(self, m, v, u=None): if u is None: u = self.fields(m) sig = self.model.transform(m) self.currentTransformedModel = sig # Ensure v is a data object. if not isinstance(v, self.dataPair): v = self.dataPair(self.survey, v) Jtv = np.zeros(self.model.nP, dtype=complex) dsig_dm = self.model.transformDeriv(m) for i, freq in enumerate(self.survey.freqs): e = u[freq, 'e'] AT = self.getA(freq).T solver = self.Solver(AT, **self.solverOpts) for txi, tx in enumerate(self.survey.getTransmitters(freq)): dMe_dsig = self.mesh.getEdgeInnerProductDeriv(sig, v=e[:,txi]) P = tx.projectFieldsDeriv(self.mesh, u) w = solver.solve(P.T * v[tx]) Jtv += - 1j*omega(freq) * ( dsig_dm.T * ( dMe_dsig.T * w ) ) return Jtv class ProblemFDEM_b(BaseProblemFDEM): """ Solving for b! """ def __init__(self, model, **kwargs): BaseProblemFDEM.__init__(self, model, **kwargs) def getA(self, freq): """ :param float freq: Frequency :rtype: scipy.sparse.csr_matrix :return: A """ mui = self.MfMui sigI = self.MeSigmaI C = self.mesh.edgeCurl return mui*C*sigI*C.T*mui + 1j*omega(freq)*mui def getRHS(self, freq): """ :param float freq: Frequency :rtype: numpy.ndarray (nE, nTx) :return: RHS """ Txs = self.survey.getTransmitters(freq) rhs = range(len(Txs)) for i, tx in enumerate(Txs): if tx.txType == 'VMD': src = Sources.MagneticDipoleVectorPotential else: raise NotImplemented('%s txType is not implemented' % tx.txType) SRCx = src(tx.loc, self.mesh.gridEx, 'x') SRCy = src(tx.loc, self.mesh.gridEy, 'y') SRCz = src(tx.loc, self.mesh.gridEz, 'z') rhs[i] = np.concatenate((SRCx, SRCy, SRCz)) a = np.concatenate(rhs).reshape((self.mesh.nE, len(Txs)), order='F') mui = self.MfMui C = self.mesh.edgeCurl b_0 = C*a return -1j*omega(freq)*mui*b_0 def calcFields(self, sol, freq): b = sol fDict = {} if 'b' in self.storeTheseFields: fDict['b'] = b if 'e' in self.storeTheseFields: e = self.MeSigmaI*self.mesh.edgeCurl.T*self.MfMui*b fDict['e'] = e return fDict def Jvec(self, m, v, u=None): if u is None: u = self.fields(m) raise NotImplemented('') # sig = self.model.transform(m) # self.currentTransformedModel = sig # Jv = self.dataPair(self.survey) # dsig_dm = self.model.transformDeriv(m) # for i, freq in enumerate(self.survey.freqs): # e = u[freq, 'e'] # A = self.getA(freq) # solver = self.Solver(A, **self.solverOpts) # for txi, tx in enumerate(self.survey.getTransmitters(freq)): # dMe_dsig = self.mesh.getEdgeInnerProductDeriv(sig, v=e[:,txi]) # P = tx.projectFieldsDeriv(self.mesh, u) # b = 1j*omega(freq) * ( dMe_dsig * ( dsig_dm * v ) ) # Ainvb = solver.solve(b) # Jv[tx] = -P*Ainvb # return Utils.mkvc(Jv) def Jtvec(self, m, v, u=None): if u is None: u = self.fields(m) # Ensure v is a data object. if not isinstance(v, self.dataPair): v = self.dataPair(self.survey, v) raise NotImplemented('') # sig = self.model.transform(m) # self.currentTransformedModel = sig # Jtv = np.zeros(self.model.nP, dtype=complex) # dsig_dm = self.model.transformDeriv(m) # for i, freq in enumerate(self.survey.freqs): # e = u[freq, 'e'] # AT = self.getA(freq).T # solver = self.Solver(AT, **self.solverOpts) # for txi, tx in enumerate(self.survey.getTransmitters(freq)): # dMe_dsig = self.mesh.getEdgeInnerProductDeriv(sig, v=e[:,txi]) # P = tx.projectFieldsDeriv(self.mesh, u) # w = solver.solve(P.T * v[tx]) # Jtv += - 1j*omega(freq) * ( dsig_dm.T * ( dMe_dsig.T * w ) ) # return Jtv