from SimPEG import Problem, Utils from SimPEG.EM.Base import BaseEMProblem from SurveyDC import Survey from FieldsDC import Fields, Fields_CC, Fields_N from SimPEG.Utils import sdiag import numpy as np from SimPEG.Utils import Zero from BoundaryUtils import getxBCyBC_CC class BaseDCProblem(BaseEMProblem): surveyPair = Survey fieldsPair = Fields Ainv = None def fields(self, m): self.curModel = m if not self.Ainv == None: self.Ainv.clean() f = self.fieldsPair(self.mesh, self.survey) A = self.getA() self.Ainv = self.Solver(A, **self.solverOpts) RHS = self.getRHS() u = self.Ainv * RHS Srcs = self.survey.srcList f[Srcs, self._solutionType] = u return f def Jvec(self, m, v, f=None): if f is None: f = self.fields(m) self.curModel = m Jv = self.dataPair(self.survey) #same size as the data A = self.getA() for src in self.survey.srcList: u_src = f[src, self._solutionType] # solution vector dA_dm_v = self.getADeriv(u_src, v) dRHS_dm_v = self.getRHSDeriv(src, v) du_dm_v = self.Ainv * ( - dA_dm_v + dRHS_dm_v ) for rx in src.rxList: df_dmFun = getattr(f, '_%sDeriv'%rx.projField, None) df_dm_v = df_dmFun(src, du_dm_v, v, adjoint=False) Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v) return Utils.mkvc(Jv) def Jtvec(self, m, v, f=None): if f is None: f = 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(m.size) AT = self.getA() for src in self.survey.srcList: u_src = f[src, self._solutionType] for rx in src.rxList: PTv = rx.evalDeriv(src, self.mesh, f, v[src, rx], adjoint=True) # wrt f, need possibility wrt m df_duTFun = getattr(f, '_%sDeriv'%rx.projField, None) df_duT, df_dmT = df_duTFun(src, None, PTv, adjoint=True) ATinvdf_duT = self.Ainv * df_duT dA_dmT = self.getADeriv(u_src, ATinvdf_duT, adjoint=True) dRHS_dmT = self.getRHSDeriv(src, ATinvdf_duT, adjoint=True) du_dmT = -dA_dmT + dRHS_dmT Jtv += df_dmT + du_dmT return Utils.mkvc(Jtv) def getSourceTerm(self): """ takes concept of source and turns it into a matrix """ """ Evaluates the sources, and puts them in matrix form :rtype: (numpy.ndarray, numpy.ndarray) :return: q (nC or nN, nSrc) """ Srcs = self.survey.srcList if self._formulation is 'EB': n = self.mesh.nN # return NotImplementedError elif self._formulation is 'HJ': n = self.mesh.nC q = np.zeros((n, len(Srcs))) for i, src in enumerate(Srcs): q[:,i] = src.eval(self) return q class Problem3D_CC(BaseDCProblem): _solutionType = 'phiSolution' _formulation = 'HJ' # CC potentials means J is on faces fieldsPair = Fields_CC def __init__(self, mesh, **kwargs): BaseDCProblem.__init__(self, mesh, **kwargs) def setBC(self): self.Div = V * self.mesh.faceDiv P_BC, B = self.mesh.getBCProjWF_simple() M = B*self.mesh.aveCC2F Grad = Div.T - P_BC*Utils.sdiag(y_BC)*M def getA(self): """ Make the A matrix for the cell centered DC resistivity problem A = D MfRhoI D^\\top V """ V = self.Vol D = V * self.mesh.faceDiv # TODO: this won't work for full anisotropy MfRhoI = self.MfRhoI A = D * MfRhoI * D.T # I think we should deprecate this for DC problem. # if self._makeASymmetric is True: # return V.T * A return A def getADeriv(self, u, v, adjoint= False): V = self.Vol D = V * self.mesh.faceDiv MfRhoIDeriv = self.MfRhoIDeriv if adjoint: # if self._makeASymmetric is True: # v = V * v return(MfRhoIDeriv( D.T * u ).T) * ( D.T * v) # I think we should deprecate this for DC problem. # if self._makeASymmetric is True: # return V.T * ( D * ( MfRhoIDeriv( D.T * ( V * u ) ) * v ) ) return D * (MfRhoIDeriv( D.T * u ) * v) def getRHS(self): """ RHS for the DC problem q """ RHS = self.getSourceTerm() # I think we should deprecate this for DC problem. # if self._makeASymmetric is True: # return self.Vol.T * RHS return RHS def getRHSDeriv(self, src, v, adjoint=False): """ Derivative of the right hand side with respect to the model """ # TODO: add qDeriv for RHS depending on m # qDeriv = src.evalDeriv(self, adjoint=adjoint) # return qDeriv return Zero() class Problem3D_N(BaseDCProblem): _solutionType = 'phiSolution' _formulation = 'EB' # N potentials means B is on faces fieldsPair = Fields_N def __init__(self, mesh, **kwargs): BaseDCProblem.__init__(self, mesh, **kwargs) def getA(self): """ Make the A matrix for the cell centered DC resistivity problem A = D MfRhoI D^\\top V """ # TODO: this won't work for full anisotropy MeSigma = self.MeSigma Grad = self.mesh.nodalGrad A = Grad.T * MeSigma * Grad # Handling Null space of A A[0,0] = A[0,0] + 1. # if self._makeASymmetric is True: # return V.T * A return A def getADeriv(self, u, v, adjoint=False): """ Product of the derivative of our system matrix with respect to the model and a vector """ MeSigma = self.MeSigma Grad = self.mesh.nodalGrad if not adjoint: return Grad.T*(self.MeSigmaDeriv(Grad*u)*v) elif adjoint: return self.MeSigmaDeriv(Grad*u).T * (Grad*v) def getRHS(self): """ RHS for the DC problem q """ RHS = self.getSourceTerm() # if self._makeASymmetric is True: # return self.Vol.T * RHS return RHS def getRHSDeriv(self, src, v, adjoint=False): """ Derivative of the right hand side with respect to the model """ # TODO: add qDeriv for RHS depending on m # qDeriv = src.evalDeriv(self, adjoint=adjoint) # return qDeriv return Zero()