示例#1
0
    def evalDeriv(self, u, v=None, adjoint=False):
        assert v is not None, 'v to multiply must be provided.'

        if not adjoint:
            data = Survey.Data(self)
            for src in self.srcList:
                for rx in src.rxList:
                    data[src, rx] = rx.evalDeriv(src, self.mesh,
                                                 self.prob.timeMesh, u, v)
            return data
        else:
            f = FieldsTDEM(self.mesh, self)
            for src in self.srcList:
                for rx in src.rxList:
                    Ptv = rx.evalDeriv(src,
                                       self.mesh,
                                       self.prob.timeMesh,
                                       u,
                                       v,
                                       adjoint=True)
                    Ptv = Ptv.reshape((-1, self.prob.timeMesh.nN), order='F')
                    if rx.projField not in f:  # first time we are projecting
                        f[src, rx.projField, :] = Ptv
                    else:  # there are already fields, so let's add to them!
                        f[src, rx.projField, :] += Ptv
            return f
示例#2
0
文件: TDEM_b.py 项目: zyex1108/simpeg
    def _AhtVec(self, m, vec):
        """
            :param numpy.array m: Conductivity model
            :param FieldsTDEM vec: Fields object
            :rtype: FieldsTDEM
            :return: f

            Multiply the matrix \\\(\\\hat{A}\\\) by a fields vector where

            .. math::
                \mathbf{\hat{A}}^\\top = \left[
                    \\begin{array}{cccc}
                        A & B & & \\\\
                          & \ddots & \ddots & \\\\
                          & & A & B \\\\
                          & & 0 & A
                    \end{array}
                \\right] \\\\
                \mathbf{A} =
                \left[
                    \\begin{array}{cc}
                        \\frac{1}{\delta t} \MfMui & \MfMui\dcurl \\\\
                        \dcurl^\\top \MfMui & -\MeSig
                    \end{array}
                \\right] \\\\
                \mathbf{B} =
                \left[
                    \\begin{array}{cc}
                        -\\frac{1}{\delta t} \MfMui & 0 \\\\
                        0 & 0
                    \end{array}
                \\right] \\\\
        """
        self.curModel = m
        f = FieldsTDEM(self.mesh, self.survey)
        for i in range(self.nT):
            b = 1.0 / self.timeSteps[
                i] * self.MfMui * vec[:, 'b', i + 1] + self.MfMui * (
                    self.mesh.edgeCurl * vec[:, 'e', i + 1])
            if i < self.nT - 1:
                b = b - 1.0 / self.timeSteps[i + 1] * self.MfMui * vec[:, 'b',
                                                                       i + 2]
            f[:, 'b', i + 1] = b
            f[:, 'e', i + 1] = self.mesh.edgeCurl.T * (
                self.MfMui * vec[:, 'b', i + 1]) - self.MeSigma * vec[:, 'e',
                                                                      i + 1]
        return f
示例#3
0
文件: TDEM_b.py 项目: zyex1108/simpeg
    def Gvec(self, m, vec, u=None):
        """
            :param numpy.array m: Conductivity model
            :param numpy.array vec: vector (like a model)
            :param FieldsTDEM u: Fields resulting from m
            :rtype: FieldsTDEM
            :return: f

            Multiply G by a vector
        """
        if u is None:
            u = self.fields(m)
        self.curModel = m

        # Note: Fields has shape (nF/E, nSrc, nT+1)
        #       However, p will only really fill (:,:,1:nT+1)
        #       meaning the 'initial fields' are zero (:,:,0)
        p = FieldsTDEM(self.mesh, self.survey)
        # 'b' at all times is zero.
        #       However, to save memory we will **not** do:
        #
        #               p[:, 'b', :] = 0.0

        # fake initial 'e' fields
        p[:, 'e', 0] = 0.0
        dMdsig = self.MeSigmaDeriv
        # self.mesh.getEdgeInnerProductDeriv(self.curModel.transform)
        # dsigdm_x_v = self.curModel.sigmaDeriv*vec
        # dsigdm_x_v = self.curModel.transformDeriv*vec
        for i in range(1, self.nT + 1):
            # TODO: G[1] may be dependent on the model
            #       for a galvanic source (deriv of the dc problem)
            #
            # Do multiplication for all src in self.survey.srcList
            for src in self.survey.srcList:
                p[src, 'e', i] = -dMdsig(u[src, 'e', i]) * vec
        return p