Files
simpeg/simpegEM/TDEM/TDEM_b.py
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2014-04-26 17:12:26 -07:00

267 lines
8.9 KiB
Python

from BaseTDEM import ProblemBaseTDEM
from SimPEG.Utils import mkvc
import numpy as np
from SurveyTDEM import SurveyTDEM1D, FieldsTDEM
class ProblemTDEM_b(ProblemBaseTDEM):
"""
Time-Domain EM problem - B-formulation
TDEM_b treats the following discretization of Maxwell's equations
.. math::
\dcurl \e^{(t+1)} + \\frac{\\b^{(t+1)} - \\b^{(t)}}{\delta t} = 0 \\\\
\dcurl^\\top \MfMui \\b^{(t+1)} - \MeSig \e^{(t+1)} = \Me \j_s^{(t+1)}
with \\\(\\b\\\) defined on cell faces and \\\(\e\\\) defined on edges.
"""
def __init__(self, mesh, mapping=None, **kwargs):
ProblemBaseTDEM.__init__(self, mesh, mapping=mapping, **kwargs)
solType = 'b'
surveyPair = SurveyTDEM1D
####################################################
# Internal Methods
####################################################
def getA(self, tInd):
"""
:param int tInd: Time index
:rtype: scipy.sparse.csr_matrix
:return: A
"""
dt = self.timeSteps[tInd]
return self.MfMui*self.mesh.edgeCurl*self.MeSigmaI*self.mesh.edgeCurl.T*self.MfMui + (1.0/dt)*self.MfMui
def getRHS(self, tInd, F):
dt = self.timeSteps[tInd]
return (1.0/dt)*self.MfMui*F.get_b(tInd-1)
####################################################
# Derivatives
####################################################
def Jvec(self, m, v, u=None):
if u is None:
u = self.fields(m)
p = self.Gvec(m, v, u)
y = self.solveAh(m, p)
return self.survey.dpred(m, u=y)
def Jtvec(self, m, v, u=None):
if u is None:
u = self.fields(m)
p = self.survey.projectFieldsAdjoint(v)
y = self.solveAht(m, p)
w = self.Gtvec(m, y, u)
return w
def Gvec(self, m, vec, u=None):
"""
:param numpy.array m: Conductivity model
:param numpy.array vec: vector (like a model)
:param simpegEM.TDEM.FieldsTDEM u: Fields resulting from m
:rtype: simpegEM.TDEM.FieldsTDEM
:return: f
Multiply G by a vector where
"""
if u is None:
u = self.fields(m)
p = FieldsTDEM(self.mesh, 1, self.nT, 'b')
curModel = self.mapping.transform(m)
c = self.mesh.getEdgeInnerProductDeriv(curModel)*self.mapping.transformDeriv(m)*vec
for i in range(self.nT):
ei = u.get_e(i)
pVal = np.empty_like(ei)
for j in range(ei.shape[1]):
pVal[:,j] = -ei[:,j]*c
p.set_e(pVal,i)
p.set_b(np.zeros((self.mesh.nF,1)), i)
return p
def Gtvec(self, m, v, u=None):
if u is None:
u = self.fields(m)
tmp = np.zeros((self.mesh.nE,self.survey.nTx))
for i in range(self.nT):
tmp += v.get_e(i)*u.get_e(i)
curModel = self.mapping.transform(m)
p = -mkvc(self.mapping.transformDeriv(m).T*self.mesh.getEdgeInnerProductDeriv(curModel).T*tmp)
return p
def solveAh(self, m, p):
def AhRHS(tInd, u):
rhs = self.MfMui*self.mesh.edgeCurl*self.MeSigmaI*p.get_e(tInd) + p.get_b(tInd)
if tInd == 0:
return rhs
dt = self.timeSteps[tInd]
return rhs + 1.0/dt*self.MfMui*u.get_b(tInd-1)
def AhCalcFields(sol, solType, tInd):
b = sol
e = self.MeSigmaI*self.mesh.edgeCurl.T*self.MfMui*b - self.MeSigmaI*p.get_e(tInd)
return {'b':b, 'e':e}
self.makeMassMatrices(m)
return self.forward(m, AhRHS, AhCalcFields)
def solveAht(self, m, p):
def AhtRHS(tInd, u):
rhs = self.MfMui*self.mesh.edgeCurl*self.MeSigmaI*p.get_e(tInd) + p.get_b(tInd)
if tInd == self.nT-1:
return rhs
dt = self.timeSteps[tInd+1]
return rhs + 1.0/dt*self.MfMui*u.get_b(tInd+1)
def AhtCalcFields(sol, solType, tInd):
b = sol
e = self.MeSigmaI*self.mesh.edgeCurl.T*self.MfMui*b - self.MeSigmaI*p.get_e(tInd)
return {'b':b, 'e':e}
self.makeMassMatrices(m)
return self.adjoint(m, AhtRHS, AhtCalcFields)
####################################################
# Functions for tests
####################################################
def AhVec(self, sigma, vec):
"""
:param numpy.array sigma: Conductivity model
:param simpegEM.TDEM.FieldsTDEM vec: Fields object
:rtype: simpegEM.TDEM.FieldsTDEM
:return: f
Multiply the matrix \\\(\\\hat{A}\\\) by a fields vector where
.. math::
\mathbf{\hat{A}} = \left[
\\begin{array}{cccc}
A & 0 & & \\\\
B & A & & \\\\
& \ddots & \ddots & \\\\
& & B & 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.makeMassMatrices(sigma)
dt = self.timeSteps[0]
b = 1.0/dt*self.MfMui*vec.get_b(0) + self.MfMui*self.mesh.edgeCurl*vec.get_e(0)
e = self.mesh.edgeCurl.T*self.MfMui*vec.get_b(0) - self.MeSigma*vec.get_e(0)
f = FieldsTDEM(self.mesh, 1, self.nT, 'b')
f.set_b(b, 0)
f.set_e(e, 0)
for i in range(1,self.nT):
dt = self.timeSteps[i]
b = 1.0/dt*self.MfMui*vec.get_b(i) + self.MfMui*self.mesh.edgeCurl*vec.get_e(i) - 1.0/dt*self.MfMui*vec.get_b(i-1)
e = self.mesh.edgeCurl.T*self.MfMui*vec.get_b(i) - self.MeSigma*vec.get_e(i)
f.set_b(b, i)
f.set_e(e, i)
return f
def AhtVec(self, sigma, vec):
"""
:param numpy.array sigma: Conductivity model
:param simpegEM.TDEM.FieldsTDEM vec: Fields object
:rtype: simpegEM.TDEM.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.makeMassMatrices(sigma)
f = FieldsTDEM(self.mesh, 1, self.nT, 'b')
for i in range(self.nT-1):
b = 1.0/self.timeSteps[i]*self.MfMui*vec.get_b(i) + self.MfMui*self.mesh.edgeCurl*vec.get_e(i) - 1.0/self.timeSteps[i+1]*self.MfMui*vec.get_b(i+1)
e = self.mesh.edgeCurl.T*self.MfMui*vec.get_b(i) - self.MeSigma*vec.get_e(i)
f.set_b(b, i)
f.set_e(e, i)
N = self.nT - 1
b = 1.0/self.timeSteps[N]*self.MfMui*vec.get_b(N) + self.MfMui*self.mesh.edgeCurl*vec.get_e(N)
e = self.mesh.edgeCurl.T*self.MfMui*vec.get_b(N) - self.MeSigma*vec.get_e(N)
f.set_b(b, N)
f.set_e(e, N)
return f
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, ncx, ncz, npad = 5., 20, 6, 20
hx = [(cs, ncx), (cs, npad, 1.3)]
hz = [(cs, npad, -1.3), (cs, ncz), (cs, npad, 1.3)]
mesh = Mesh.CylMesh([hx,1,hz], '00C')
mapping = Maps.Vertical1DMap(mesh)
opts = {'txLoc':0.,
'txType':'VMD_MVP',
'rxLoc':np.r_[150., 0., 0.],
'rxType':'bz',
'timeCh':np.logspace(-4,-2,20),
}
survey = EM.TDEM.SurveyTDEM1D(**opts)
prb = EM.TDEM.ProblemTDEM_b(mesh, mapping=mapping)
# prb.setTimes([1e-5, 5e-5, 2.5e-4], [150, 150, 150])
# prb.setTimes([1e-5, 5e-5, 2.5e-4], [10, 10, 10])
prb.timeSteps = [(1e-5, 10)]
prb.pair(survey)
sigma = np.random.rand(mesh.nCz)
print survey.dpred(sigma)