from SimPEG import Problem, Solver import numpy as np from scipy.constants import mu_0 from SimPEG.Utils import sdiag, mkvc from FieldsFDEM import FieldsFDEM from DataFDEM import DataFDEM class ProblemFDEM_e(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, mesh, model, **kwargs): Problem.BaseProblem.__init__(self, mesh, model, **kwargs) solType = 'b' storeTheseFields = 'e' dataPair = DataFDEM solveOpts = {'factorize':False, 'backend':'scipy'} j_s = None def getFieldsObject(self): F = FieldsFDEM(self.mesh, self.data.nTx, self.data.nFreq, store=self.storeTheseFields) return F #################################################### # Mass Matrices #################################################### @property def MfMui(self): return self._MfMui @property def Me(self): return self._Me @property def MeSigma(self): return self._MeSigma @property def MeSigmaI(self): return self._MeSigmaI def makeMassMatrices(self, m): #TODO: hardcoded to sigma as the model sigma = self.model.transform(m) self._Me = self.mesh.getEdgeInnerProduct() self._MeSigma = self.mesh.getEdgeInnerProduct(sigma) # TODO: this will not work if tensor conductivity self._MeSigmaI = sdiag(1/self.MeSigma.diagonal()) #TODO: assuming constant mu self._MfMui = self.mesh.getFaceInnerProduct(1/mu_0) #################################################### # Internal Methods #################################################### def getA(self, freqInd): """ :param int tInd: Time index :rtype: scipy.sparse.csr_matrix :return: A """ omega = self.data.omega[freqInd] return self.mesh.edgeCurl.T*self.MfMui*self.mesh.edgeCurl + 1j*omega*self.MeSigma def getRHS(self, freqInd): omega = self.data.omega[freqInd] return -1j*omega*self.Me*self.j_s def fields(self, m, useThisRhs=None): RHS = useThisRhs or self.getRHS self.makeMassMatrices(m) F = self.getFieldsObject() for freqInd in range(self.data.nFreq): A = self.getA(freqInd) b = self.getRHS(freqInd) e = Solver(A, options=self.solveOpts).solve(b) F.set_e(e, freqInd) omega = self.data.omega[freqInd] #TODO: check if mass matrices needed: b = -1./(1j*omega)*self.mesh.edgeCurl*e F.set_b(b, freqInd) return F def Jvec(self, m, v, u=None): if u is None: u = self.fields(m) raise NotImplementedError('Jvec todo!') def Jtvec(self, m, v, u=None): if u is None: u = self.fields(m) raise NotImplementedError('Jtvec todo!') if __name__ == '__main__': from SimPEG import * import simpegEM as EM from simpegEM.Utils.Ana import hzAnalyticDipoleT from scipy.constants import mu_0 import matplotlib.pyplot as plt cs = 5. ncx = 6 ncy = 6 ncz = 6 npad = 3 hx = Utils.meshTensors(((npad,cs), (ncx,cs), (npad,cs))) hy = Utils.meshTensors(((npad,cs), (ncy,cs), (npad,cs))) hz = Utils.meshTensors(((npad,cs), (ncz,cs), (npad,cs))) mesh = Mesh.TensorMesh([hx,hy,hz]) XY = Utils.ndgrid(np.linspace(20,50,3), np.linspace(20,50,3)) rxLoc = np.c_[XY, np.ones(XY.shape[0])*40] model = Model.LogModel(mesh) opts = {'txLoc':0., 'txType':'VMD_MVP', 'rxLoc': rxLoc, 'rxType':'bz', 'freq': np.logspace(0,3,4), } dat = EM.FDEM.DataFDEM(**opts) prb = EM.FDEM.ProblemFDEM_e(mesh, model) prb.pair(dat) sigma = np.log(np.ones(mesh.nC)*1e-3) j_sx = np.zeros(mesh.vnEx) j_sx[6,6,6] = 1 j_s = np.r_[Utils.mkvc(j_sx),np.zeros(mesh.nEy+mesh.nEz)] prb.j_s = j_s f = prb.fields(sigma) colorbar(mesh.plotSlice((f.get_e(3)), 'E', ind=11, normal='Z', view='real')[0]) plt.show()