mirror of
https://github.com/wassname/simpeg.git
synced 2026-06-28 23:26:19 +08:00
Rowan Cockett
279 lines
8.7 KiB
Python
279 lines
8.7 KiB
Python
from SimPEG import Survey, Problem, Utils, np, sp, Solver as SimpegSolver
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from scipy.constants import mu_0
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from SurveyMT import SurveyMT, FieldsMT
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def omega(freq):
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"""Change frequency to angular frequency, omega"""
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return 2.*np.pi*freq
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class MTProblem(Problem.BaseProblem):
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def __init__(self, mesh, **kwargs):
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Problem.BaseProblem.__init__(self, mesh, **kwargs)
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solType = 'e'
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storeTheseFields = ['e', 'b']
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surveyPair = SurveyMT
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dataPair = Survey.Data
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Solver = SimpegSolver
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solverOpts = {}
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####################################################
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# Mass Matrices
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####################################################
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@property
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def MfMui(self):
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#TODO: assuming constant mu
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if getattr(self, '_MfMui', None) is None:
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self._MfMui = self.mesh.getFaceInnerProduct(1/mu_0)
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return self._MfMui
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@property
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def Me(self):
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if getattr(self, '_Me', None) is None:
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self._Me = self.mesh.getEdgeInnerProduct()
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return self._Me
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@property
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def MeSigma(self):
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#TODO: hardcoded to sigma as the model
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if getattr(self, '_MeSigma', None) is None:
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sigma = self.curTModel
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self._MeSigma = self.mesh.getEdgeInnerProduct(sigma)
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return self._MeSigma
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# TODO:
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# MeSigmaBG
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@property
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def MeSigmaI(self):
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#TODO: hardcoded to sigma as the model
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if getattr(self, '_MeSigmaI', None) is None:
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sigma = self.curTModel
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self._MeSigmaI = self.mesh.getEdgeInnerProduct(sigma, invMat=True)
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return self._MeSigmaI
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curModel = Utils.dependentProperty('_curModel', None, ['_MeSigma', '_MeSigmaI', '_curTModel', '_curTModelDeriv'], 'Sets the current model, and removes dependent mass matrices.')
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@property
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def curTModel(self):
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if getattr(self, '_curTModel', None) is None:
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self._curTModel = self.mapping.transform(self.curModel)
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return self._curTModel
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@property
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def curTModelDeriv(self):
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if getattr(self, '_curTModelDeriv', None) is None:
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self._curTModelDeriv = self.mapping.transformDeriv(self.curModel)
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return self._curTModelDeriv
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def fields(self, m):
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self.curModel = m
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RHS, CalcFields = self.getRHS, self.calcFields
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F = FieldsMT(self.mesh, self.survey)
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for freq in self.survey.freqs:
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A = self.getA(freq)
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rhs = RHS(freq)
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Ainv = self.Solver(A, **self.solverOpts)
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e = Ainv * rhs # is this e?
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Src = self.survey.getSources(freq)
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F[Src, 'e'] = e
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F[Src, 'b'] = self.mesh.edgeCurl * e # ???
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return F
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def getA(self, freq):
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"""
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:param float freq: Frequency
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:rtype: scipy.sparse.csr_matrix
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:return: A
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"""
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mui = self.MfMui
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sig = self.MeSigma
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C = self.mesh.edgeCurl
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return C.T*mui*C + 1j*omega(freq)*sig
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def getAbg(self, freq):
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"""
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:param float freq: Frequency
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:rtype: scipy.sparse.csr_matrix
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:return: A
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"""
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mui = self.MfMui
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sigBG = self.MeSigmaBG
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C = self.mesh.edgeCurl
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return C.T*mui*C + 1j*omega(freq)*sigBG
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def getADeriv(self, freq, u, v, adjoint=False):
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sig = self.curTModel
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dsig_dm = self.curTModelDeriv
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dMe_dsig = self.mesh.getEdgeInnerProductDeriv(sig, v=u)
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if adjoint:
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return 1j * omega(freq) * ( dsig_dm.T * ( dMe_dsig.T * v ) )
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return 1j * omega(freq) * ( dMe_dsig * ( dsig_dm * v ) )
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def getRHS(self, freq):
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"""
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:param float freq: Frequency
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:rtype: numpy.ndarray (nE, 2)
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:return: one RHS for both polarizations
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"""
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raise NotImplementedError()
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getAbg(freq)
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"""
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Put this in MT.Sources.EldadsSource
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from simpegMT.Utils import get1DEfields
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# Get a 1d solution for a halfspace background
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mesh1d = simpeg.Mesh.TensorMesh([M.hz],np.array([M.x0[2]]))
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e0_1d = get1DEfields(mesh1d,M.r(sigBG,'CC','CC','M')[0,0,:],freq)
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# Setup x (east) polarization (_x)
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ex_x = np.zeros(M.vnEx,dtype=complex)
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ey_x = np.zeros((M.nEy,1),dtype=complex)
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ez_x = np.zeros((M.nEz,1),dtype=complex)
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# Assign the source to ex_x
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for i in arange(M.vnEx[0]):
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for j in arange(M.vnEx[2]):
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ex_x[i,j,:] = e0_1d
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eBG_x = np.vstack((simpeg.Utils.mkvc(M.r(ex_x,'Ex','Ex','V'),2),ey_x,ez_x))
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rhs_x = ABG.dot(eBG_x)
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"""
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Txs = self.survey.getTransmitters(freq)
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# assert that only one Tx/src?
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# Create the two polarizations at this freq and return np array (nE,2).
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# solve analytic.... get p1 p2
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# Abg * [p1,p2] = rhs
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rhs = range(len(Txs))
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for i, tx in enumerate(Txs):
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if tx.txType == 'VMD': # EH source.
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src = Sources.MagneticDipoleVectorPotential # this is where you would put multiple types of boundary conditions.
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else:
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raise NotImplemented('%s txType is not implemented' % tx.txType)
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SRCx = src(tx.loc, self.mesh.gridEx, 'x')
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SRCy = src(tx.loc, self.mesh.gridEy, 'y')
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SRCz = src(tx.loc, self.mesh.gridEz, 'z')
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rhs[i] = np.concatenate((SRCx, SRCy, SRCz))
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a = np.concatenate(rhs).reshape((self.mesh.nE, len(Txs)), order='F')
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mui = self.MfMui
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C = self.mesh.edgeCurl
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j_s = C.T*mui*C*a
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return -1j*omega(freq)*j_s
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##################################################################
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# Inversion stuff
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##################################################################
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# Not really used now....
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def calcFields(self, sol, freq, fieldType, adjoint=False):
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e = sol
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if fieldType == 'e':
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return e
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elif fieldType == 'b':
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if not adjoint:
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b = -(1./(1j*omega(freq))) * ( self.mesh.edgeCurl * e )
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else:
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b = -(1./(1j*omega(freq))) * ( self.mesh.edgeCurl.T * e )
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return b
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raise NotImplementedError('fieldType "%s" is not implemented.' % fieldType)
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def calcFieldsDeriv(self, sol, freq, fieldType, v, adjoint=False):
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e = sol
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if fieldType == 'e':
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return None
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elif fieldType == 'b':
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return None
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raise NotImplementedError('fieldType "%s" is not implemented.' % fieldType)
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def Jvec(self, m, v, u=None):
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if u is None:
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u = self.fields(m)
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self.curModel = m
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Jv = self.dataPair(self.survey)
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for freq in self.survey.freqs:
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A = self.getA(freq)
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solver = self.Solver(A, **self.solverOpts)
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for tx in self.survey.getTransmitters(freq):
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u_tx = u[tx, self.solType]
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w = self.getADeriv(freq, u_tx, v)
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Ainvw = solver.solve(w)
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for rx in tx.rxList:
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fAinvw = self.calcFields(Ainvw, freq, rx.projField)
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P = lambda v: rx.projectFieldsDeriv(tx, self.mesh, u, v)
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df_dm = self.calcFieldsDeriv(u_tx, freq, rx.projField, v)
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if df_dm is None:
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Jv[tx, rx] = - P(fAinvw)
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else:
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Jv[tx, rx] = - P(fAinvw) + P(df_dm)
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return Utils.mkvc(Jv)
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def Jtvec(self, m, v, u=None):
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if u is None:
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u = self.fields(m)
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self.curModel = m
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# Ensure v is a data object.
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if not isinstance(v, self.dataPair):
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v = self.dataPair(self.survey, v)
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Jtv = np.zeros(self.mapping.nP)
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for freq in self.survey.freqs:
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AT = self.getA(freq).T
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solver = self.Solver(AT, **self.solverOpts)
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for tx in self.survey.getTransmitters(freq):
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u_tx = u[tx, self.solType]
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for rx in tx.rxList:
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PTv = rx.projectFieldsDeriv(tx, self.mesh, u, v[tx, rx], adjoint=True)
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fPTv = self.calcFields(PTv, freq, rx.projField, adjoint=True)
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w = solver.solve( fPTv )
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Jtv_rx = - self.getADeriv(freq, u_tx, w, adjoint=True)
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df_dm = self.calcFieldsDeriv(u_tx, freq, rx.projField, PTv, adjoint=True)
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if df_dm is not None:
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Jtv_rx += df_dm
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real_or_imag = rx.projComp
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if real_or_imag == 'real':
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Jtv += Jtv_rx.real
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elif real_or_imag == 'imag':
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Jtv += - Jtv_rx.real
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else:
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raise Exception('Must be real or imag')
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return Jtv
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