Files
simpeg/simpegMT/ProblemMT.py
T
2015-05-07 19:22:28 -07:00

152 lines
4.5 KiB
Python

from SimPEG import Survey, Problem, Utils, Models, np, sp, SolverLU as SimpegSolver
from simpegEM.FDEM import BaseFDEMProblem
from simpegEM.Utils import omega
from scipy.constants import mu_0
from SurveyMT import SurveyMT, FieldsMT
import multiprocessing, sys, time
class BaseMTProblem(BaseFDEMProblem):
def __init__(self, mesh, **kwargs):
BaseFDEMProblem.__init__(self, mesh, **kwargs)
surveyPair = SurveyMT
dataPair = Survey.Data
Solver = SimpegSolver
solverOpts = {}
verbose = False
# Notes:
# Use the forward and devs from BaseFDEMProblem
# Might need to add more stuff here.
@property
def MeSigmaBG(self):
#TODO: hardcoded to sigma as the model
if getattr(self, '_MeSigmaBG', None) is None:
sigmaBG = self.backModel
self._MeSigmaBG = self.mesh.getEdgeInnerProduct(sigmaBG)
return self._MeSigmaBG
class ProblemMT_eForm_ps(BaseMTProblem):
"""
A MT problem solving a e formulation and a primary/secondary fields decompostion.
Solves the equation
"""
_fieldType = 'e'
_eqLocs = 'FE'
fieldsPair = FieldsMT
# Set new properties
# Background model
@property
def backModel(self):
"""
Sets the model, and removes dependent mass matrices.
"""
return getattr(self, '_backModel', None)
@backModel.setter
def backModel(self, value):
if value is self.backModel:
return # it is the same!
self._backModel = Models.Model(value, self.mapping)
for prop in self.deleteTheseOnModelUpdate:
if hasattr(self, prop):
delattr(self, prop)
def __init__(self, mesh, **kwargs):
BaseMTProblem.__init__(self, mesh, **kwargs)
def getA(self, freq):
"""
Function to get the A matrix.
:param float freq: Frequency
:rtype: scipy.sparse.csr_matrix
:return: A
"""
mui = self.MfMui
sig = self.MeSigma
C = self.mesh.edgeCurl
return C.T*mui*C + 1j*omega(freq)*sig
def getADeriv(self, freq, u, v, adjoint=False):
sig = self.curTModel
dsig_dm = self.curTModelDeriv
dMe_dsig = self.mesh.getEdgeInnerProductDeriv(sig, v=u)
if adjoint:
return 1j * omega(freq) * ( dsig_dm.T * ( dMe_dsig.T * v ) )
return 1j * omega(freq) * ( dMe_dsig * ( dsig_dm * v ) )
def getRHS(self, freq, backSigma):
"""
Function to return the right hand side for the system.
:param float freq: Frequency
:param numpy.ndarray (nC,) backSigma: Background conductivity model
:rtype: numpy.ndarray (nE, 2)
:return: one RHS for both polarizations
"""
# Get sources for the frequency
src = self.survey.getSources(freq)
# Make sure that there is 2 polarizations.
# assert len()
# Get the background electric fields
from simpegMT.Sources import homo1DModelSource
eBG_bp = homo1DModelSource(self.mesh,freq,backSigma)
deltM = self.curModel - self.backModel
Abg = -1j*omega(freq)*deltM*eBG_bp
return Abg*eBG_bp, eBG_bp
def getRHSderiv(self, freq, backSigma, u, v, adjoint=False):
raise NotImplementedError('getRHSDeriv not implemented yet')
return None
def fields(self, m, m_back):
'''
Function to calculate all the fields for the model m.
:param np.ndarray (nC,) m: Conductivity model
:param np.ndarray (nC,) m_back: Background conductivity model
'''
self.curModel = m
self.backModel = m_back
# RHS, CalcFields = self.getRHS(freq,m_back), self.calcFields
F = FieldsMT(self.mesh, self.survey)
if verbose:
startTime = time.time()
print 'Starting work for {:.3e}'.format(freq)
sys.stdout.flush()
A = self.getA(freq)
rhs, e_p = self.getRHS(freq,m_back)
Ainv = self.Solver(A, **self.solverOpts)
e_s = Ainv * rhs
e = e_p + e_s
# Store the fields
Src = self.survey.getSources(freq)
# Store the fieldss
F[Src, 'e_px'] = e[:,0]
F[Src, 'e_py'] = e[:,1]
# Note curl e = -iwb so b = -curl/iw
b = -( self.mesh.edgeCurl * e )/( 1j*omega(freq) )
F[Src, 'b_px'] = b[:,0]
F[Src, 'b_py'] = b[:,1]
if verbose:
print 'Ran for {:f} seconds'.format(time.time()-startTime)
sys.stdout.flush()
return F