start of Casing analytic and test

This commit is contained in:
Lindsey Heagy
2015-05-06 06:47:53 -07:00
parent 96b0d6a38c
commit 1e52c365bc
4 changed files with 152 additions and 1 deletions
+91
View File
@@ -0,0 +1,91 @@
from SimPEG import Utils, np
from scipy.constants import mu_0, epsilon_0
from simpegEM.Utils.EMUtils import k
def getKc(freq,sigma,a,b,mu=mu_0,eps=epsilon_0):
a = float(a)
b = float(b)
return 2. * np.sqrt(b / a) * np.exp(-1j*k(freq,sigma,mu,eps)*(b-a))
def _r2(xyz):
return np.sum(xyz**2,1)
def _getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1.):
Kc1 = getKc(freq,sigma[1],a,b,mu,eps)
nobs = obsloc.shape[0]
dxyz = obsloc - np.c_[np.ones(nobs)]*np.r_[srcloc]
r2 = _r2(dxyz[:,:2])
sqrtr2z2 = np.sqrt(r2 + dxyz[:,2]**2)
k2 = k(freq,sigma[2],mu,eps)
return Kc1 * moment / (4.*np.pi) *np.exp(-1j*k2*sqrtr2z2) / sqrtr2z2
def _getCasingHertzMagDipoleDeriv_r(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1.):
HertzZ = _getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
nobs = obsloc.shape[0]
dxyz = obsloc - np.c_[np.ones(nobs)]*np.r_[srcloc]
r2 = _r2(dxyz[:,:2])
sqrtr2z2 = np.sqrt(r2 + dxyz[:,2]**2)
k2 = k(freq,sigma[2],mu,eps)
return -HertzZ * np.sqrt(r2) / sqrtr2z2 * (1j*k2 + 1./ sqrtr2z2)
def _getCasingHertzMagDipoleDeriv_z(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1.):
HertzZ = _getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
nobs = obsloc.shape[0]
dxyz = obsloc - np.c_[np.ones(nobs)]*np.r_[srcloc]
r2z2 = _r2(dxyz)
sqrtr2z2 = np.sqrt(r2z2)
k2 = k(freq,sigma[2],mu,eps)
return -HertzZ*dxyz[:,2] /sqrtr2z2 * (1j*k2 + 1./sqrtr2z2)
def _getCasingHertzMagDipole2Deriv_z_r(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1.):
HertzZ = _getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
dHertzZdr = _getCasingHertzMagDipoleDeriv_r(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
nobs = obsloc.shape[0]
dxyz = obsloc - np.c_[np.ones(nobs)]*np.r_[srcloc]
r2 = _r2(dxyz[:,:2])
r = np.sqrt(r2)
z = dxyz[:,2]
sqrtr2z2 = np.sqrt(r2 + z**2)
k2 = k(freq,sigma[2],mu,eps)
return dHertzZdr*(-z/sqrtr2z2)*(1j*k2+1./sqrtr2z2) + HertzZ*(z*r/sqrtr2z2**3)*(1j*k2 + 2./sqrtr2z2)
def _getCasingHertzMagDipole2Deriv_z_z(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1.):
HertzZ = _getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
dHertzZdz = _getCasingHertzMagDipoleDeriv_z(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
nobs = obsloc.shape[0]
dxyz = obsloc - np.c_[np.ones(nobs)]*np.r_[srcloc]
r2 = _r2(dxyz[:,:2])
r = np.sqrt(r2)
z = dxyz[:,2]
sqrtr2z2 = np.sqrt(r2 + z**2)
k2 = k(freq,sigma[2],mu,eps)
return (dHertzZdz*z + HertzZ)/sqrtr2z2*(-1j*k2 - 1./sqrtr2z2) + HertzZ*z/sqrtr2z2**3*(1j*k2*z + 2.*z/sqrtr2z2)
def getCasingEphiMagDipole(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1):
return 1j * omega(freq) * mu * _getCasingHertzMagDipoleDeriv_r(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
def getCasingHrMagDipole(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1):
return _getCasingHertzMagDipole2Deriv_z_r(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
def getCasingHzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu=mu_0,eps=epsilon_0,moment=1):
d2HertzZdz2 = _getCasingHertzMagDipole2Deriv_z_z(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
k2 = k(freq,sigma[2],mu,eps)
HertzZ(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
return d2HertzZdz2 + k2**2 * HertzZ
+1
View File
@@ -1,2 +1,3 @@
from TDEM import hzAnalyticDipoleT
from FDEM import hzAnalyticDipoleF
from FDEMcasing import *
+59
View File
@@ -0,0 +1,59 @@
from SimPEG import Tests, Utils, np
import simpegEM.Analytics.FDEMcasing as Casing
import unittest
n = 50.
freq = 1.
a = 5e-2
b = a + 1e-2
sigma = np.r_[1., 5.5e6, 1e-1]
srcloc = np.r_[0., 0., 0.]
xobs = np.random.rand(n)+10.
yobs = np.zeros(n)
zobs = np.random.randn(n)
plotit = False
def CasingMagDipoleDeriv_r(x):
obsloc = np.vstack([x, yobs, zobs]).T
f = Casing._getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b)
g = Utils.sdiag(Casing._getCasingHertzMagDipoleDeriv_r(srcloc,obsloc,freq,sigma,a,b))
return f,g
def CasingMagDipoleDeriv_z(z):
obsloc = np.vstack([xobs, yobs, z]).T
f = Casing._getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b)
g = Utils.sdiag(Casing._getCasingHertzMagDipoleDeriv_z(srcloc,obsloc,freq,sigma,a,b))
return f,g
def CasingMagDipole2Deriv_z_r(x):
obsloc = np.vstack([x, yobs, zobs]).T
f = Casing._getCasingHertzMagDipoleDeriv_z(srcloc,obsloc,freq,sigma,a,b)
g = Utils.sdiag(Casing._getCasingHertzMagDipole2Deriv_z_r(srcloc,obsloc,freq,sigma,a,b))
return f,g
def CasingMagDipole2Deriv_z_z(z):
obsloc = np.vstack([xobs, yobs, z]).T
f = Casing._getCasingHertzMagDipoleDeriv_z(srcloc,obsloc,freq,sigma,a,b)
g = Utils.sdiag(Casing._getCasingHertzMagDipole2Deriv_z_z(srcloc,obsloc,freq,sigma,a,b))
return f,g
class Casing_DerivTest(unittest.TestCase):
Tests.checkDerivative(CasingMagDipoleDeriv_r,np.ones(n)*10+np.random.randn(n),plotIt=False)
Tests.checkDerivative(CasingMagDipoleDeriv_z,np.random.randn(n),plotIt=False)
Tests.checkDerivative(CasingMagDipole2Deriv_z_r,np.ones(n)*10+np.random.randn(n),plotIt=False)
Tests.checkDerivative(CasingMagDipole2Deriv_z_z,np.random.randn(n),plotIt=False)
if __name__ == '__main__':
unittest.main()
+1 -1
View File
@@ -11,7 +11,7 @@ class FieldsTest(unittest.TestCase):
srcLoc = np.r_[0,0,0.]
rxList0 = EM.FDEM.RxFDEM(XYZ, 'exi')
Src0 = EM.FDEM.SrcFDEM_MagDipole(srcLoc, 3., [rxList0])
rxList1 = EM.FDEM.RxFDEM(XYZ, 'bxi')
rxList1 = EM.FDEM.RxFDEM(XYZ, 'bxi')
Src1 = EM.FDEM.SrcFDEM_MagDipole(srcLoc, 3., [rxList1])
rxList2 = EM.FDEM.RxFDEM(XYZ, 'bxi')
Src2 = EM.FDEM.SrcFDEM_MagDipole(srcLoc, 2., [rxList2])