from SimPEG import Survey, Utils, Problem, np, sp, mkvc from scipy.constants import mu_0 import sys from numpy.lib import recfunctions as recFunc from simpegEM.Utils.EMUtils import omega ############## ### Fields ### ############## class FieldsMT(Problem.Fields): """Field Storage for a MT survey.""" knownFields = {} dtype = complex class FieldsMT_1D(FieldsMT): """ Fields storage for the 1D MT solution. """ knownFields = {'e_1dSolution':'F'} aliasFields = { 'e_1d' : ['e_1dSolution','F','_e'], 'e_1dPrimary' : ['e_1dSolution','F','_ePrimary'], 'e_1dSecondary' : ['e_1dSolution','F','_eSecondary'], 'b_1d' : ['e_1dSolution','E','_b'], 'b_1dPrimary' : ['e_1dSolution','E','_bPrimary'], 'b_1dSecondary' : ['e_1dSolution','E','_bSecondary'] } def __init__(self,mesh,survey,**kwargs): FieldsMT.__init__(self,mesh,survey,**kwargs) def _ePrimary(self, eSolution, srcList): ePrimary = np.zeros_like(eSolution) for i, src in enumerate(srcList): ep = src.ePrimary(self.survey.prob) if ep is not None: ePrimary[:,i] = ep[:,-1] return ePrimary def _eSecondary(self, eSolution, srcList): return eSolution def _e(self, eSolution, srcList): return self._ePrimary(eSolution,srcList) + self._eSecondary(eSolution,srcList) def _eDeriv_u(self, src, v, adjoint = False): return None def _eDeriv_m(self, src, v, adjoint = False): # assuming primary does not depend on the model return None def _bPrimary(self, eSolution, srcList): bPrimary = np.zeros([self.survey.mesh.nE,eSolution.shape[1]], dtype = complex) for i, src in enumerate(srcList): bp = src.bPrimary(self.survey.prob) if bp is not None: bPrimary[:,i] += bp[:,-1] return bPrimary def _bSecondary(self, eSolution, srcList): C = self.mesh.nodalGrad b = (C * eSolution) for i, src in enumerate(srcList): b[:,i] *= - 1./(1j*omega(src.freq)) # There is no magnetic source in the MT problem # S_m, _ = src.eval(self.survey.prob) # if S_m is not None: # b[:,i] += 1./(1j*omega(src.freq)) * S_m return b def _b(self, eSolution, srcList): return self._bPrimary(eSolution, srcList) + self._bSecondary(eSolution, srcList) def _bSecondaryDeriv_u(self, src, v, adjoint = False): C = self.mesh.nodalGrad if adjoint: return - 1./(1j*omega(src.freq)) * (C.T * v) return - 1./(1j*omega(src.freq)) * (C * v) def _bSecondaryDeriv_m(self, src, v, adjoint = False): # Doesn't depend on m # _, S_eDeriv = src.evalDeriv(self.survey.prob, adjoint) # S_eDeriv = S_eDeriv(v) # if S_eDeriv is not None: # return 1./(1j * omega(src.freq)) * S_eDeriv return None def _bDeriv_u(self, src, v, adjoint=False): # Primary does not depend on u return self._bSecondaryDeriv_u(src, v, adjoint) def _bDeriv_m(self, src, v, adjoint=False): # Assuming the primary does not depend on the model return self._bSecondaryDeriv_m(src, v, adjoint) def _fDeriv_u(self, src, v, adjoint=False): """ Derivative of the fields object wrt u. :param MTsrc src: MT source :param numpy.ndarray v: random vector of f_sol.size This function stacks the fields derivatives appropriately return a vector of size (nreEle+nrbEle) """ de_du = v #Utils.spdiag(np.ones((self.nF,))) db_du = self._bDeriv_u(src, v, adjoint) # Return the stack # This doesn't work... return np.vstack((de_du,db_du)) def _fDeriv_m(self, src, v, adjoint=False): """ Derivative of the fields object wrt m. This function stacks the fields derivatives appropriately """ return None class FieldsMT_3D(FieldsMT): """ Fields storage for the 3D MT solution. """ knownFields = {'e_px':'E','e_py':'E','b_px':'F','b_py':'F'} aliasFields = { } # 'e_1d' : ['e_1dSolution','F','_e'], # 'e_1dPrimary' : ['e_1dSolution','F','_ePrimary'], # 'e_1dSecondary' : ['e_1dSolution','F','_eSecondary'], # 'b_1d' : ['e_1dSolution','E','_b'], # 'b_1dPrimary' : ['e_1dSolution','E','_bPrimary'], # 'b_1dSecondary' : ['e_1dSolution','E','_bSecondary'] # }