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simpeg/SimPEG/Examples/MT_1D_analytic_nlayer_Earth.py
T
GudniRos cf5181016f Made MT_1d_analytic_nLayer_Earth.run have default n layers of 3. 
Trying to fix example testing.
2016-06-07 09:45:02 -07:00

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from scipy.constants import epsilon_0, mu_0
import matplotlib.pyplot as plt
import numpy as np
from ipywidgets import *
from SimPEG.EM.Utils import k, omega
"""
MT1D: n layered earth problem
*****************************
Author: Thibaut Astic
Contact: thast@eos.ubc.ca
Date: January 2016
This code compute the analytic response of a n-layered Earth to a plane wave (Magneto-Tellurics).
We start by looking at Maxwell's equations in the electric
field \\\(\\\mathbf{E}\\) and the magnetic flux
\\\(\\\mathbf{H}\\) to write the wave equations
\\(\\ \nabla ^2 \mathbf{E_x} + k^2 \mathbf{E_x} = 0 \\) &
\\(\\ \nabla ^2 \mathbf{H_y} + k^2 \mathbf{H_y} = 0 \\)
Then solving the equations in each layer "j" between z_{j-1} and z_j in the form of
\\(\\ E_{x,j} (z) = U_j e^{i k (z-z_{j-1})} + D_j e^{-i k (z-z_{j-1})} \\)
\\(\\ H_{y,j} (z) = \frac{1}{Z_j} (D_j e^{-i k (z-z_{j-1})} - U_j e^{i k (z-z_{j-1})}) \\)
With U and D the Up and Down components of the E-field.
The iteration from one layer to another is ensure by:
\\(\\ \left(\begin{matrix} E_{x,j} \\ H_{y,j} \end{matrix} \right) =
P_j T_j P^{-1}_J \left(\begin{matrix} E_{x,j+1} \\ H_{y,j+1} \end{matrix} \right) \\)
And the Boundary Condition is set for the E-field in the last layer, with no Up component (=0)
and only a down component (=1 then normalized by the highest amplitude to ensure numeric stability)
The layer 0 is assumed to be the air layer.
"""
#Define a frquency range for a survey
frange = lambda minfreq, maxfreq, step: np.logspace(minfreq,maxfreq,num = step, base = 10.)
#Functions to create random physical Perties for a n-layered earth
thick = lambda minthick, maxthick, nlayer: np.append(np.array([1.2*10.**5]),
np.ndarray.round(minthick + (maxthick-minthick)* np.random.rand(nlayer-1,1)
,decimals =1))
sig = lambda minsig, maxsig, nlayer: np.append(np.array([0.]),
np.ndarray.round(10.**minsig + (10.**maxsig-10.**minsig)* np.random.rand(nlayer,1)
,decimals=3))
mu = lambda minmu, maxmu, nlayer: np.append(np.array([1.]),
np.ndarray.round(minmu + (maxmu-minmu)* np.random.rand(nlayer,1)
,decimals=1))
eps = lambda mineps, maxeps, nlayer: np.append(np.array([1.]),
np.ndarray.round(mineps + (maxeps-mineps)* np.random.rand(nlayer,1)
,decimals=1))
#Evaluate Impedance Z of a layer
ImpZ = lambda f, mu, k: omega(f)*mu*mu_0/k
#Complex Cole-Cole Conductivity - EM utils
PCC= lambda siginf,m,t,c,f: siginf*(1.-(m/(1.+(1j*omega(f)*t)**c)))
#Converted thickness array into top of layer array
top = lambda thick: np.cumsum(thick)
#Propagation Matrix and theirs inverses
#matrix T for transition of Up and Down components accross a layer
T = lambda h,k: np.matrix([[np.exp(1j*k*h),0.],[0.,np.exp(-1j*k*h)]],dtype='complex_')
Tinv = lambda h,k: np.matrix([[np.exp(-1j*k*h),0.],[0.,np.exp(1j*k*h)]],dtype='complex_')
#transition of Up and Down components accross a layer
UD_Z = lambda UD,z,zj,k : T((z-zj),k)*UD
#matrix P relating Up and Down components with E and H fields
P = lambda z: np.matrix([[1.,1,],[-1./z,1./z]],dtype='complex_')
Pinv = lambda z: np.matrix([[1.,-z],[1.,z]],dtype='complex_')/2.
#Time Variation of E and H
E_ZT = lambda U,D,f,t : np.exp(1j*omega(f)*t)*(U+D)
H_ZT = lambda U,D,Z,f,t : (1./Z)*np.exp(1j*omega(f)*t)*(D-U)
#Plot the configuration of the problem
def PlotConfiguration(thick,sig,eps,mu,ax,widthg,z):
topn = top(thick)
widthn = np.arange(-widthg,widthg+widthg/10.,widthg/10.)
ax.set_ylim([z.min(),z.max()])
ax.set_xlim([-widthg,widthg])
ax.set_ylabel("Depth (m)", fontsize=16.)
ax.yaxis.tick_right()
ax.yaxis.set_label_position("right")
#define filling for the different layers
hatches=['/' , '+', 'x', '|' , '\\', '-' , 'o' , 'O' , '.' , '*' ]
#Write the physical properties of air
ax.annotate(("Air, $\sigma$ =%1.0f mS/m")%(sig[0]*10**(3)),
xy=(-widthg/2., -np.abs(z.max())/2.), xycoords='data',
xytext=(-widthg/2., -np.abs(z.max())/2.), textcoords='data',
fontsize=14.)
ax.annotate(("$\epsilon_r$= %1i")%(eps[0]),
xy=(-widthg/2., -np.abs(z.max())/3.), xycoords='data',
xytext=(-widthg/2., -np.abs(z.max())/3.), textcoords='data',
fontsize=14.)
ax.annotate(("$\mu_r$= %1i")%(mu[0]),
xy=(-widthg/2., -np.abs(z.max())/3.), xycoords='data',
xytext=(0, -np.abs(z.max())/3.), textcoords='data',
fontsize=14.)
#Write the physical properties of the differents layers up to the (n-1)-th and fill it with pattern
for i in range(1,len(topn)-1,1):
if topn[i] == topn[i+1]:
pass
else:
ax.annotate(("$\sigma$ =%3.3f mS/m")%(sig[i]*10**(3)),
xy=(0., (2.*topn[i]+topn[i+1])/3), xycoords='data',
xytext=(0., (2.*topn[i]+topn[i+1])/3), textcoords='data',
fontsize=14.)
ax.annotate(("$\epsilon_r$= %1i")%(eps[i]),
xy=(-widthg/1.1, (2.*topn[i]+topn[i+1])/3), xycoords='data',
xytext=(-widthg/1.1, (2.*topn[i]+topn[i+1])/3), textcoords='data',
fontsize=14.)
ax.annotate(("$\mu_r$= %1.2f")%(mu[i]),
xy=(-widthg/2., (2.*topn[i]+topn[i+1])/3), xycoords='data',
xytext=(-widthg/2., (2.*topn[i]+topn[i+1])/3), textcoords='data',
fontsize=14.)
ax.plot(widthn,topn[i]*np.ones_like(widthn),color='black')
ax.fill_between(widthn,topn[i],topn[i+1],alpha=0.3,color="none",edgecolor='black', hatch=hatches[(i-1)%10])
#Write the physical properties of the n-th layer and fill it with pattern
ax.plot(widthn,topn[-1]*np.ones_like(widthn),color='black')
ax.fill_between(widthn,topn[-1],z.max(),alpha=0.3,color="none",edgecolor='black', hatch=hatches[(len(topn)-2)%10])
ax.annotate(("$\sigma$ =%3.3f mS/m")%(sig[-1]*10**(3)),
xy=(0., (2.*topn[-1]+z.max())/3), xycoords='data',
xytext=(0., (2.*topn[-1]+z.max())/3), textcoords='data',
fontsize=14.)
ax.annotate(("$\epsilon_r$= %1i")%(eps[-1]),
xy=(-widthg/1.1, (2.*topn[-1]+z.max())/3), xycoords='data',
xytext=(-widthg/1.1, (2.*topn[-1]+z.max())/3), textcoords='data',
fontsize=14.)
ax.annotate(("$\mu_r$= %1.2f")%(mu[-1]),
xy=(-widthg/2., (2.*topn[-1]+z.max())/3), xycoords='data',
xytext=(-widthg/2., (2.*topn[-1]+z.max())/3), textcoords='data',
fontsize=14.)
#plot Trees!
ax.annotate("",
xy=(widthg/2., -1.*z.max()/5.), xycoords='data',
xytext=(widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.2,head_length=1.2',color='green',linewidth=2.)
)
ax.annotate("",
xy=(widthg/2., -3./4.*z.max()/5.), xycoords='data',
xytext=(widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.4,head_length=1.4',color='green',linewidth=2.)
)
ax.annotate("",
xy=(widthg/2., -1./2.*z.max()/5.), xycoords='data',
xytext=(widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.6,head_length=1.6',color='green',linewidth=2.)
)
ax.annotate("",
xy=(1.2*widthg/2., -1.*z.max()/5.), xycoords='data',
xytext=(1.2*widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.2,head_length=1.2',color='green',linewidth=2.)
)
ax.annotate("",
xy=(1.2*widthg/2., -3./4.*z.max()/5.), xycoords='data',
xytext=(1.2*widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.4,head_length=1.4',color='green',linewidth=2.)
)
ax.annotate("",
xy=(1.2*widthg/2., -1./2.*z.max()/5.), xycoords='data',
xytext=(1.2*widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.6,head_length=1.6',color='green',linewidth=2.)
)
ax.annotate("",
xy=(1.5*widthg/2., -1.*z.max()/5.), xycoords='data',
xytext=(1.5*widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.2,head_length=1.2',color='green',linewidth=2.)
)
ax.annotate("",
xy=(1.5*widthg/2., -3./4.*z.max()/5.), xycoords='data',
xytext=(1.5*widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.4,head_length=1.4',color='green',linewidth=2.)
)
ax.annotate("",
xy=(1.5*widthg/2., -1./2.*z.max()/5.), xycoords='data',
xytext=(1.5*widthg/2., 0.), textcoords='data',
arrowprops=dict(arrowstyle='->, head_width=1.6,head_length=1.6',color='green',linewidth=2.)
)
ax.invert_yaxis()
return ax
#Propagate Up and Down component for a certain frequency & evaluate E and H field
def Propagate(f,H,sig,chg,taux,c,mu,eps,n):
sigcm = np.zeros_like(sig,dtype='complex_')
for j in range(1,len(sig)):
sigcm[j]=PCC(sig[j],chg[j],taux[j],c[j],f)
K = k(f, sigcm, mu, eps)
Z = ImpZ(f,mu,K)
EH = np.matrix(np.zeros((2,n+1),dtype = 'complex_'),dtype = 'complex_')
UD = np.matrix(np.zeros((2,n+1),dtype = 'complex_'),dtype = 'complex_')
UD[1,-1] = 1.
for i in range(-2,-(n+2),-1):
UD[:,i] = Tinv(H[i+1],K[i])*Pinv(Z[i])*P(Z[i+1])*UD[:,i+1]
UD = UD/((np.abs(UD[0,:]+UD[1,:])).max())
for j in range(0,n+1):
EH[:,j] = np.matrix([[1.,1,],[-1./Z[j],1./Z[j]]])*UD[:,j]
return UD, EH, Z ,K
#Evaluate the apparent resistivity and phase for a frequency range
def appres(F,H,sig,chg,taux,c,mu,eps,n):
Res = np.zeros_like(F)
Phase = np.zeros_like(F)
App_ImpZ= np.zeros_like(F,dtype='complex_')
for i in range(0,len(F)):
UD,EH,Z ,K = Propagate(F[i],H,sig,chg,taux,c,mu,eps,n)
App_ImpZ[i] = EH[0,1]/EH[1,1]
Res[i] = np.abs(App_ImpZ[i])**2./(mu_0*omega(F[i]))
Phase[i] = np.angle(App_ImpZ[i], deg = True)
return Res,Phase
#Evaluate Up, Down components, E and H field, for a frequency range,
#a discretized depth range and a time range (use to calculate envelope)
def calculateEHzt(F,H,sig,chg,taux,c,mu,eps,n,zsample,tsample):
topc = top(H)
layer = np.zeros(len(zsample),dtype=np.int)-1
Exzt = np.matrix(np.zeros((len(zsample),len(tsample)),dtype = 'complex_'),dtype = 'complex_')
Hyzt = np.matrix(np.zeros((len(zsample),len(tsample)),dtype = 'complex_'),dtype = 'complex_')
Uz = np.matrix(np.zeros((len(zsample),len(tsample)),dtype = 'complex_'),dtype = 'complex_')
Dz = np.matrix(np.zeros((len(zsample),len(tsample)),dtype = 'complex_'),dtype = 'complex_')
UDaux = np.matrix(np.zeros((2,len(zsample)),dtype = 'complex_'),dtype = 'complex_')
for i in range(0,n+1,1):
layer = layer+(zsample>=topc[i])*1
for j in range(0,len(F)):
UD,EH,Z ,K = Propagate(F[j],H,sig,chg,taux,c,mu,eps,n)
for p in range(0,len(zsample)):
UDaux[:,p] = UD_Z(UD[:,layer[p]],zsample[p],topc[layer[p]],K[layer[p]])
for q in range(0,len(tsample)):
Exzt[p,q] = Exzt[p,q] + E_ZT(UDaux[0,p],UDaux[1,p],F[j],tsample[q])/len(F)
Hyzt[p,q] = Hyzt[p,q] + H_ZT(UDaux[0,p],UDaux[1,p],Z[layer[p]],F[j],tsample[q])/len(F)
Uz[p,q] = Uz[p,q] + UDaux[0,p]*np.exp(1j*omega(F[j])*tsample[q])/len(F)
Dz[p,q] = Dz[p,q] + UDaux[1,p]*np.exp(1j*omega(F[j])*tsample[q])/len(F)
return Exzt,Hyzt,Uz,Dz,UDaux,layer
#Function to Plot Apparent Resistivity and Phase
def PlotAppRes(F,H,sig,chg,taux,c,mu,eps,n,fenvelope,PlotEnvelope):
Res, Phase = appres(F,H,sig,chg,taux,c,mu,eps,n)
fig,ax = plt.subplots(1,2,figsize=(16,10))
ax[0].scatter(Res,F,color='black')
ax[0].set_xscale('Log')
ax[0].set_yscale('Log')
ax[0].set_xlim([10.**(np.log10(Res.min())-1.),10.**(np.log10(Res.max())+1.)])
ax[0].set_ylim([F.min(),F.max()])
ax[0].set_xlabel('Apparent Resistivity (Ohm*m)',fontsize=16.,color="black")
ax[0].set_ylabel('Frequency (Hz)',fontsize=16.)
ax[0].grid(which='major')
ax0 = ax[0].twiny()
ax0.set_xlim([0.,90.])
ax0.set_ylim([F.min(),F.max()])
ax0.scatter(Phase,F,color='purple')
ax0.set_xlabel('Phase (Degrees)',fontsize=16.,color="purple")
zc=np.arange(-(H[1:].max()+10)*n,(H[1:].max()+10)*n,10.)
ax[0].tick_params(labelsize=16)
ax[1].tick_params(labelsize=16)
ax0.tick_params(labelsize=16)
if PlotEnvelope:
widthn=np.logspace(np.log10(Res.min())-1., np.log10(Res.max())+1., num=100, endpoint=True, base=10.0)
fenvelope1n=np.ones(100)*fenvelope
ax[0].plot(widthn,fenvelope1n,linestyle='dashed',color='black')
tc=np.arange(0.,1./fenvelope,0.01/(fenvelope))
Exzt,Hyzt,Uz,Dz,UDaux,layer = calculateEHzt(np.array([fenvelope]),H,sig,chg,taux,c,mu,eps,n,zc,tc)
ax1=ax[1].twiny()
ax[1].tick_params(labelsize=16)
ax1.tick_params(labelsize=16)
ax[1].set_xlabel('Amplitude Electric Field E (V/m)',color='blue',fontsize=16)
ax1.set_xlabel('Amplitude Magnetic Field H (A/m)',color='red',fontsize=16)
ax[1].fill_betweenx(zc,np.squeeze(np.asarray(np.real(Exzt.min(axis=1)))),
np.squeeze(np.asarray(np.real(Exzt.max(axis=1)))),
color='blue', alpha=0.1)
ax1.fill_betweenx(zc,np.squeeze(np.asarray(np.real(Hyzt.min(axis=1)))),
np.squeeze(np.asarray(np.real(Hyzt.max(axis=1)))),
color='red', alpha=0.1)
ax[1] = PlotConfiguration(H,sig,eps,mu,ax[1],(1.5*np.abs(Exzt).max()),zc)
ax1.set_xlim([-1.5*np.abs(Hyzt).max(),1.5*np.abs(Hyzt).max()])
ax1.set_xlim([-1.5*np.abs(Hyzt).max(),1.5*np.abs(Hyzt).max()])
else:
print 'No envelop (if True, might be slow)'
ax[1] = PlotConfiguration(H,sig,eps,mu,ax[1],1.,zc)
ax[1].get_xaxis().set_ticks([])
plt.show()
#Interactive MT for Notebook
def PlotAppRes3LayersInteract(h1,h2,sigl1,sigl2,sigl3,mul1,mul2,mul3,epsl1,epsl2,epsl3,PlotEnvelope,F_Envelope):
frangn=frange(-5,5,100.)
sig3= np.array([0.,0.001,0.1, 0.001])
thick3 = np.array([120000.,50.,50.])
eps3=np.array([1.,1.,1.,1])
mu3=np.array([1.,1.,1.,1])
chg3=np.array([0.,0.1,0.,0.2])
chg3_0=np.array([0.,0.1,0.,0.])
taux3=np.array([0.,0.1,0.,0.1])
c3=np.array([1.,1.,1.,1.])
sig3[1]=sigl1
sig3[1]=10.**sig3[1]
sig3[2]=sigl2
sig3[2]=10.**sig3[2]
sig3[3]=sigl3
sig3[3]=10.**sig3[3]
mu3[1]=mul1
mu3[2]=mul2
mu3[3]=mul3
eps3[1]=epsl1
eps3[2]=epsl2
eps3[3]=epsl3
thick3[1]=h1
thick3[2]=h2
PlotAppRes(frangn,thick3,sig3,chg3_0,taux3,c3,mu3,eps3,3,F_Envelope,PlotEnvelope)
def run(n=3,plotIt=True):
# something to make a plot
F = frange(-5.,5.,20)
H = thick(50.,100.,n)
sign = sig(-5.,0.,n)
mun = mu(1.,2.,n)
epsn = eps(1.,9.,n)
chg = np.zeros_like(sign)
taux = np.zeros_like(sign)
c = np.zeros_like(sign)
Res, Phase = appres(F,H,sign,chg,taux,c,mun,epsn,n)
if plotIt:
PlotAppRes(F, H, sign, chg, taux, c, mun, epsn, n, fenvelope=1000., PlotEnvelope=True)
return Res, Phase
if __name__ == '__main__':
run()
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