Files
simpeg/SimPEG/MT/Utils/MT1Dsolutions.py
Rowan Cockett 558e8879fe SimPEG.MT Mergify.
Merge branch 'move2Simpeg' of https://github.com/simpeg/simpegmt into mt/dev

Conflicts:
	.gitignore
	.travis.yml
	LICENSE
	docs/conf.py
	docs/index.rst
	requirements.txt
	setup.py
2016-01-14 15:36:58 -08:00

46 lines
1.3 KiB
Python

import numpy as np, SimPEG as simpeg
from MT1Danalytic import getEHfields
from scipy.constants import mu_0
def get1DEfields(m1d,sigma,freq,sourceAmp=1.0):
"""Function to get 1D electrical fields"""
# Get the gradient
G = m1d.nodalGrad
# Mass matrices
# Magnetic permeability
Mmu = simpeg.Utils.sdiag(m1d.vol*(1.0/mu_0))
# Conductivity
Msig = m1d.getFaceInnerProduct(sigma)
# Set up the solution matrix
A = G.T*Mmu*G + 1j*2.*np.pi*freq*Msig
# Define the inner part of the solution matrix
Aii = A[1:-1,1:-1]
# Define the outer part of the solution matrix
Aio = A[1:-1,[0,-1]]
# Set the boundary conditions
Ed, Eu, Hd, Hu = getEHfields(m1d,sigma,freq,m1d.vectorNx)
Etot = (Ed + Eu)
if sourceAmp is not None:
Etot = ((Etot/Etot[-1])*sourceAmp) # Scale the fields to be equal to sourceAmp at the top
## Note: The analytic solution is derived with e^iwt
bc = np.r_[Etot[0],Etot[-1]]
# The right hand side
rhs = Aio*bc
# Solve the system
Aii_inv = simpeg.Solver(Aii)
eii = Aii_inv*rhs
# Assign the boundary conditions
e = np.r_[bc[0],eii,bc[1]]
# Return the electrical fields
return e
if __name__ == '__main__':
hz = [(100.,18)]
M = simpeg.Mesh.TensorMesh([hz],'C')
sig = np.zeros(M.nC) + 1e-8
sig[M.vectorCCx<=0] = sigHalf