Futurize 1, futurize 2, pasteurize.

This commit is contained in:
Brendan Smithyman
2016-07-16 14:17:02 -05:00
parent 362975d2bd
commit ca8d8f8c2d
197 changed files with 2618 additions and 1235 deletions
+12 -4
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@@ -1,3 +1,11 @@
from __future__ import division
from __future__ import unicode_literals
from __future__ import print_function
from __future__ import absolute_import
from future import standard_library
standard_library.install_aliases()
from builtins import range
from past.utils import old_div
import numpy as np
from scipy.constants import mu_0, pi
from scipy import special
@@ -24,8 +32,8 @@ def DCAnalyticHalf(txloc, rxlocs, sigma, earth_type="wholespace"):
rM = np.sqrt( (M[:,0]-txloc[0])**2 + (M[:,1]-txloc[1])**2 + (M[:,2]-txloc[1])**2 )
rN = np.sqrt( (N[:,0]-txloc[0])**2 + (N[:,1]-txloc[1])**2 + (N[:,2]-txloc[1])**2 )
phiM = 1./(4*np.pi*rM*sigma)
phiN = 1./(4*np.pi*rN*sigma)
phiM = old_div(1.,(4*np.pi*rM*sigma))
phiN = old_div(1.,(4*np.pi*rN*sigma))
phi = phiM - phiN
if earth_type == "halfspace":
@@ -69,8 +77,8 @@ def DCAnalyticSphere(txloc, rxloc, xc, radius, sigma, sigma1, \
Pleg.append(special.legendre(i, monic=0))
rho = 1./sigma
rho1 = 1./sigma1
rho = old_div(1.,sigma)
rho1 = old_div(1.,sigma1)
# Center of the sphere should be aligned in txloc in y-direction
yc = txloc[1]
+5
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@@ -1,4 +1,9 @@
from __future__ import division
from __future__ import unicode_literals
from __future__ import print_function
from __future__ import absolute_import
from future import standard_library
standard_library.install_aliases()
import numpy as np
from scipy.constants import mu_0, pi
from scipy.special import erf
+5
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@@ -1,4 +1,9 @@
from __future__ import division
from __future__ import unicode_literals
from __future__ import print_function
from __future__ import absolute_import
from future import standard_library
standard_library.install_aliases()
import numpy as np
from scipy.constants import mu_0, pi, epsilon_0
from scipy.special import erf
+12 -5
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@@ -1,3 +1,10 @@
from __future__ import division
from __future__ import unicode_literals
from __future__ import print_function
from __future__ import absolute_import
from future import standard_library
standard_library.install_aliases()
from past.utils import old_div
from SimPEG import Utils, np
from scipy.constants import mu_0, epsilon_0
from SimPEG.EM.Utils.EMUtils import k
@@ -6,7 +13,7 @@ def getKc(freq,sigma,a,b,mu=mu_0,eps=epsilon_0):
a = float(a)
b = float(b)
# return 1./(2*np.pi) * np.sqrt(b / a) * np.exp(-1j*k(freq,sigma,mu,eps)*(b-a))
return np.sqrt(b / a) * np.exp(-1j*k(freq,sigma,mu,eps)*(b-a))
return np.sqrt(old_div(b, a)) * np.exp(-1j*k(freq,sigma,mu,eps)*(b-a))
def _r2(xyz):
return np.sum(xyz**2,1)
@@ -34,7 +41,7 @@ def _getCasingHertzMagDipoleDeriv_r(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.ones
sqrtr2z2 = np.sqrt(r2 + dxyz[:,2]**2)
k2 = k(freq,sigma[2],mu[2],eps)
return -HertzZ * np.sqrt(r2) / sqrtr2z2 * (1j*k2 + 1./ sqrtr2z2)
return -HertzZ * np.sqrt(r2) / sqrtr2z2 * (1j*k2 + old_div(1., sqrtr2z2))
def _getCasingHertzMagDipoleDeriv_z(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.ones(3),eps=epsilon_0,moment=1.):
@@ -47,7 +54,7 @@ def _getCasingHertzMagDipoleDeriv_z(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.ones
sqrtr2z2 = np.sqrt(r2z2)
k2 = k(freq,sigma[2],mu[2],eps)
return -HertzZ*dxyz[:,2] /sqrtr2z2 * (1j*k2 + 1./sqrtr2z2)
return -HertzZ*dxyz[:,2] /sqrtr2z2 * (1j*k2 + old_div(1.,sqrtr2z2))
def _getCasingHertzMagDipole2Deriv_z_r(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.ones(3),eps=epsilon_0,moment=1.):
HertzZ = _getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
@@ -62,7 +69,7 @@ def _getCasingHertzMagDipole2Deriv_z_r(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.o
sqrtr2z2 = np.sqrt(r2 + z**2)
k2 = k(freq,sigma[2],mu[2],eps)
return dHertzZdr*(-z/sqrtr2z2)*(1j*k2+1./sqrtr2z2) + HertzZ*(z*r/sqrtr2z2**3)*(1j*k2 + 2./sqrtr2z2)
return dHertzZdr*(old_div(-z,sqrtr2z2))*(1j*k2+old_div(1.,sqrtr2z2)) + HertzZ*(z*r/sqrtr2z2**3)*(1j*k2 + old_div(2.,sqrtr2z2))
def _getCasingHertzMagDipole2Deriv_z_z(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.ones(3),eps=epsilon_0,moment=1.):
HertzZ = _getCasingHertzMagDipole(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
@@ -77,7 +84,7 @@ def _getCasingHertzMagDipole2Deriv_z_z(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.o
sqrtr2z2 = np.sqrt(r2 + z**2)
k2 = k(freq,sigma[2],mu[2],eps)
return (dHertzZdz*z + HertzZ)/sqrtr2z2*(-1j*k2 - 1./sqrtr2z2) + HertzZ*z/sqrtr2z2**3*(1j*k2*z + 2.*z/sqrtr2z2)
return (dHertzZdz*z + HertzZ)/sqrtr2z2*(-1j*k2 - old_div(1.,sqrtr2z2)) + HertzZ*z/sqrtr2z2**3*(1j*k2*z + 2.*z/sqrtr2z2)
def getCasingEphiMagDipole(srcloc,obsloc,freq,sigma,a,b,mu=mu_0*np.ones(3),eps=epsilon_0,moment=1.):
return 1j * omega(freq) * mu * _getCasingHertzMagDipoleDeriv_r(srcloc,obsloc,freq,sigma,a,b,mu,eps,moment)
+11 -4
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@@ -1,12 +1,19 @@
from __future__ import division
from __future__ import unicode_literals
from __future__ import print_function
from __future__ import absolute_import
from future import standard_library
standard_library.install_aliases()
from past.utils import old_div
import numpy as np
from scipy.constants import mu_0, pi
from scipy.special import erf
def hzAnalyticDipoleT(r, t, sigma):
theta = np.sqrt((sigma*mu_0)/(4*t))
theta = np.sqrt(old_div((sigma*mu_0),(4*t)))
tr = theta*r
etr = erf(tr)
t1 = (9/(2*tr**2) - 1)*etr
t2 = (1/np.sqrt(pi))*(9/tr + 4*tr)*np.exp(-tr**2)
hz = (t1 - t2)/(4*pi*r**3)
t1 = (old_div(9,(2*tr**2)) - 1)*etr
t2 = (old_div(1,np.sqrt(pi)))*(old_div(9,tr) + 4*tr)*np.exp(-tr**2)
hz = old_div((t1 - t2),(4*pi*r**3))
return hz
+11 -5
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@@ -1,5 +1,11 @@
from TDEM import hzAnalyticDipoleT
from FDEM import hzAnalyticDipoleF
from FDEMcasing import *
from DC import DCAnalyticHalf, DCAnalyticSphere
from FDEMDipolarfields import *
from __future__ import absolute_import
from __future__ import unicode_literals
from __future__ import print_function
from __future__ import division
from future import standard_library
standard_library.install_aliases()
from .TDEM import hzAnalyticDipoleT
from .FDEM import hzAnalyticDipoleF
from .FDEMcasing import *
from .DC import DCAnalyticHalf, DCAnalyticSphere
from .FDEMDipolarfields import *