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Author SHA1 Message Date
Lindsey Heagy 3cbefac3ba try using list for Jv instead of datapair - has been seen to cause memory leaks 2016-06-29 15:55:34 -07:00
Lindsey Heagy e7e497a06d don't use Zero() in mapping derivs) 2016-06-29 08:45:45 -07:00
Lindsey Heagy 3157aa02cf naming update 2016-06-28 08:15:19 -07:00
Lindsey Heagy c40d11ef53 - better model for testing Parametric casing map
- allow vector containing values in the inactive set to be passed (not just nC in length)
2016-06-26 15:24:33 -07:00
Lindsey Heagy c75e3d0246 use a dictionary to keep track of parametric model parameters. Test mappings on cyl meshes, parametric casing and layer model 2016-06-25 16:51:18 -07:00
Lindsey Heagy 14f0d90f99 debugging derivs 2016-06-23 13:06:15 -07:00
Lindsey Heagy 425b1e292c only accept one source for the prim-sec source 2016-06-21 18:00:41 -07:00
Lindsey Heagy f6cd8696d1 call fields inside of SrcDeriv for primsec 2016-06-21 17:36:53 -07:00
Lindsey Heagy f788d5f05d bug hunting a silly memory issue (don't add vectors to column arrays!). return sparse matrices from mapping derivs for multiplying things 2016-06-21 17:20:02 -07:00
Lindsey Heagy 1521b08af6 remove @property from projPrimary 2016-05-31 23:48:04 -07:00
Lindsey Heagy 8c366463e7 call projection with problem 2016-05-31 23:19:02 -07:00
Lindsey Heagy 6d77ae9a12 pass problem to projection matrix in primsecsrc 2016-05-31 23:08:57 -07:00
Lindsey Heagy ce88c676d4 add a projection map (for re-arranging models)
use current sigmaModel in src
2016-05-31 22:44:39 -07:00
Lindsey Heagy 1e6ed86135 - parametrized layer
- parameterized block in layer inherits parametrized layer
2016-05-31 21:39:59 -07:00
Lindsey Heagy 9061ef5839 start of including primary fields derivs 2016-05-31 21:04:26 -07:00
Lindsey Heagy 0638fa308c start of prim sec src with more derivs 2016-05-30 20:30:00 -07:00
Lindsey Heagy 54478ad05e don't use adjoint when not asking for the adjoint! 2016-05-30 11:40:42 -07:00
Lindsey Heagy 2cf0edb736 bug fix in PrimSec src Deriv 2016-05-30 11:29:24 -07:00
Lindsey Heagy 3b5dfecb46 cleanup imports and class instantiation of prim-sec src in sigma 2016-05-30 10:05:15 -07:00
Lindsey Heagy 93d8ef5921 don't need m on the prim-sec src 2016-05-30 09:37:06 -07:00
Lindsey Heagy 5b0a58b751 typo in src input 2016-05-30 09:26:28 -07:00
Lindsey Heagy 9155a9c474 prim sec src in conductivity 2016-05-30 09:10:53 -07:00
Lindsey Heagy 64510bc606 Merge branch 'dev' into maps/feat-parametrizedBlock 2016-05-29 14:51:11 -07:00
Lindsey 09eb2106ec Merge pull request #307 from simpeg/ref/dev
Ref/dev
2016-05-29 14:50:43 -07:00
Lindsey Heagy d9f0241da3 typo fix in nC (it is mesh.nC) 2016-05-29 14:21:08 -07:00
Lindsey Heagy 9a7225c9f6 - bug fix in parametrized block when active cells are used - need a shape
- add a pole receiver for DC
2016-05-29 13:40:21 -07:00
Lindsey Heagy e8e022fcc6 return a scipy sparse matrix for the deriv (a bit silly - it is dense, but nicer for multiplication). Init Regularization with a nP 2016-05-28 15:40:28 -07:00
Lindsey Heagy 341b98d23a use layer center and layer thickness to parametrize layer 2016-05-28 13:06:19 -07:00
D Fournier 406703f1c6 Merge branch 'dev' into ref/dev
Conflicts:
	docs/examples/DC_Forward_PseudoSection.rst
2016-05-27 11:10:39 -07:00
D Fournier 7b72d3a92d Merge branch 'dev' into ref/dev
Conflicts:
	SimPEG/DCIP/DCIPUtils.py
2016-05-27 10:01:28 -07:00
Lindsey Heagy efbc8f9057 add docs for ParametrizedBlockInLayer, moved docs from rst to python files and automodule the docs for maps 2016-05-26 23:06:57 -07:00
Lindsey Heagy 39ece11d8a Merge branch 'dev' into maps/feat-parametrizedBlock 2016-05-26 21:32:57 -07:00
Lindsey cf89f5f6a2 Merge pull request #322 from simpeg/bug/propmap
Bug/propmap
2016-05-26 20:52:42 -07:00
Lindsey Heagy aa1086eba3 use fixed prop map in EM 2016-05-26 18:03:09 -07:00
Lindsey Heagy 1c53129da6 fix bug in prop map linked derivs 2016-05-26 17:58:30 -07:00
sgkang 6fd3be77de Merge pull request #304 from simpeg/dcip/dev
Dcip/dev
2016-05-26 13:27:44 -07:00
Lindsey Heagy c36b5a600d add parametrized block in a layer map 2016-05-26 10:30:10 -07:00
Lindsey Heagy 0379df2bf2 attempt to clean up docs in DCIP utils 2016-05-04 22:27:02 -07:00
Lindsey Heagy 66440b0478 add depreciation warnings to DCIP utils for activeind from topo 2016-05-04 22:14:41 -07:00
Lindsey Heagy dbdcc3cefb use sigma in MfRhoDeriv - due to propmap bug 2016-05-04 22:06:32 -07:00
Lindsey Heagy dd45a6a085 name updates in DC_Forward_PseudoSection, DC_Utils, example for Utils_surface2ind_topo 2016-05-02 11:40:02 -07:00
Lindsey Heagy ba8f270b3a start of surface2ind_topo 2016-05-01 13:17:16 -07:00
Lindsey Heagy 4257ea77b3 remove InjectActiveCellsTopo. you should use InjectActiveCells 2016-04-29 15:09:04 -07:00
Lindsey Heagy a0174e4f30 kwarg name updates 2016-04-29 12:52:45 -07:00
24 changed files with 1381 additions and 550 deletions
+157 -196
View File
@@ -1,12 +1,16 @@
from SimPEG import np
from SimPEG import np, Utils
import BaseDC as DC
import BaseDC as IP
import warnings
def getActiveindfromTopo(mesh, topo):
# def genActiveindfromTopo(mesh, topo):
"""
Get active indices from topography
"""
warnings.warn(
"`getActiveindfromTopo` is deprecated and will be removed in future versions. Use `SimPEG.Utils.surface2ind_topo` instead",
FutureWarning)
from scipy.interpolate import NearestNDInterpolator
if mesh.dim==3:
nCxy = mesh.nCx*mesh.nCy
@@ -28,6 +32,9 @@ def gettopoCC(mesh, airind):
"""
Get topography from active indices of mesh.
"""
warnings.warn(
"`gettopoCC` is deprecated and will be removed in future versions. Use `SimPEG.Utils.surface2ind_topo` instead",
FutureWarning)
mesh2D = Mesh.TensorMesh([mesh.hx, mesh.hy], mesh.x0[:2])
zc = mesh.gridCC[:,2]
AIRIND = airind.reshape((mesh.vnC[0]*mesh.vnC[1],mesh.vnC[2]), order='F')
@@ -118,34 +125,27 @@ def readUBC_DC3Dobstopo(filename,mesh,topo,probType="CC"):
def readUBC_DC2DModel(fileName):
"""
Read UBC GIF 2DTensor model and generate 2D Tensor model in simpeg
Read UBC GIF 2DTensor model and generate 2D Tensor model in simpeg
Input:
:param fileName, path to the UBC GIF 2D model file
Output:
:param SimPEG TensorMesh 2D object
:return
Created on Thu Nov 12 13:14:10 2015
@author: dominiquef
:param string fileName: path to the UBC GIF 2D model file
:rtype: TensorMesh
:return: SimPEG TensorMesh 2D object
"""
from SimPEG import np, mkvc
# Open fileand skip header... assume that we know the mesh already
obsfile = np.genfromtxt(fileName,delimiter=' \n',dtype=np.str,comments='!')
obsfile = np.genfromtxt(fileName, delimiter=' \n', dtype=np.str, comments='!')
dim = np.array(obsfile[0].split(),dtype=float)
dim = np.array(obsfile[0].split(), dtype=float)
temp = np.array(obsfile[1].split(),dtype=float)
temp = np.array(obsfile[1].split(), dtype=float)
if len(temp) > 1:
model = np.zeros(dim)
for ii in range(len(obsfile)-1):
mm = np.array(obsfile[ii+1].split(),dtype=float)
mm = np.array(obsfile[ii+1].split(), dtype=float)
model[:,ii] = mm
model = model[:,::-1]
@@ -153,10 +153,10 @@ def readUBC_DC2DModel(fileName):
else:
if len(obsfile[1:])==1:
mm = np.array(obsfile[1:].split(),dtype=float)
mm = np.array(obsfile[1:].split(), dtype=float)
else:
mm = np.array(obsfile[1:],dtype=float)
mm = np.array(obsfile[1:], dtype=float)
# Permute the second dimension to flip the order
model = mm.reshape(dim[1],dim[0])
@@ -169,23 +169,19 @@ def readUBC_DC2DModel(fileName):
return model
def plot_pseudoSection(DCsurvey, axs, stype='dpdp', dtype="appc", clim=None, cblabel=True, axlabel = True, colorbar = True, contour = None):
def plot_pseudoSection(DCsurvey, axs, surveyType='dipole-dipole', unitType='volt', clim=None, cblabel=True, axlabel = True, colorbar = True, contour = None):
"""
Read list of 2D tx-rx location and plot a speudo-section of apparent
resistivity.
Read list of 2D tx-rx location and plot a speudo-section of apparent
resistivity.
Assumes flat topo for now...
Assumes flat topo for now...
Input:
:param d2D, z0
:switch stype -> Either 'pdp' (pole-dipole) | 'dpdp' (dipole-dipole)
:switch dtype=-> Either 'appr' (app. res) | 'appc' (app. con) | 'volt' (potential)
Output:
:figure scatter plot overlayed on image
Edited Feb 17th, 2016
@author: dominiquef
:param SurveyDC DCsurvey:
:param string surveyType: Either 'pole-dipole' | 'dipole-dipole'
:param string unitType: Either 'appResistivity' | 'appConductivity' | 'volt'
:rtype: matplotlib.plt
:return: figure scatter plot overlayed on image
"""
from SimPEG import np
@@ -218,39 +214,39 @@ def plot_pseudoSection(DCsurvey, axs, stype='dpdp', dtype="appc", clim=None, cbl
Cmid = (Tx[0][0] + Tx[1][0])/2
Pmid = (Rx[0][:,0] + Rx[1][:,0])/2
# Change output for dtype
if dtype == 'volt':
# Change output for unitType
if unitType == 'volt':
rho = np.hstack([rho,data])
else:
# Compute pant leg of apparent rho
if stype == 'pdp':
if surveyType == 'pole-dipole':
leg = data * 2*np.pi * MA * ( MA + MN ) / MN
elif stype == 'dpdp':
elif surveyType == 'dipole-dipole':
leg = data * 2*np.pi / ( 1/MA - 1/MB - 1/NB + 1/NA )
else:
print """dtype must be 'pdp'(pole-dipole) | 'dpdp' (dipole-dipole) """
print """unitType must be 'pole-dipole' | 'dipole-dipole' """
break
if dtype == 'appc':
if unitType == 'appConductivity':
leg = np.log10(abs(1./leg))
rho = np.hstack([rho,leg])
elif dtype == 'appr':
elif unitType == 'appResistivity':
leg = np.log10(abs(leg))
rho = np.hstack([rho,leg])
else:
print """dtype must be 'appr' | 'appc' | 'volt' """
print """unitType must be 'appResistivity' | 'appConductivity' | 'volt' """
break
midx = np.hstack([midx, ( Cmid + Pmid )/2 ])
@@ -259,7 +255,7 @@ def plot_pseudoSection(DCsurvey, axs, stype='dpdp', dtype="appc", clim=None, cbl
# Grid points
grid_x, grid_z = np.mgrid[np.min(midx):np.max(midx), np.min(midz):np.max(midz)]
grid_rho = griddata(np.c_[midx,midz], rho.T, (grid_x, grid_z), method='linear')
# Scale the color scheme
if clim == None:
vmin, vmax = rho.min(), rho.max()
@@ -268,36 +264,37 @@ def plot_pseudoSection(DCsurvey, axs, stype='dpdp', dtype="appc", clim=None, cbl
# Plot data
grid_rho = np.ma.masked_where(np.isnan(grid_rho), grid_rho)
ph = plt.pcolormesh(grid_x[:,0],grid_z[0,:],grid_rho.T, vmin = vmin, vmax = vmax)
plt.gca().tick_params(axis='both', which='major', labelsize=8)
if contour is not None:
plt.contour(grid_x,grid_z,grid_rho,levels = contour,colors = 'r', vmin = vmin, vmax = vmax)
# Add scatter points
axs.scatter(midx,midz,s=10,c=rho.T, vmin = vmin, vmax = vmax)
if colorbar:
if dtype == 'volt':
if unitType == 'volt':
cbar = plt.colorbar(ph, ax = axs, format="%4.1f",fraction=0.04,orientation="horizontal")
else:
else:
cbar = plt.colorbar(ph, ax = axs, format="$10^{%.1f}$",fraction=0.04,orientation="horizontal")
cmin,cmax = cbar.get_clim()
ticks = np.linspace(cmin,cmax,3)
cbar.set_ticks(ticks)
cbar.ax.tick_params(labelsize=10)
if cblabel:
if dtype == 'appc':
cbar.set_label("App.Cond",size=12)
elif dtype == 'appr':
cbar.set_label("App.Res.",size=12)
elif dtype == 'volt':
cbar.set_label("Potential (V)",size=12)
cmin,cmax = cbar.get_clim()
ticks = np.linspace(cmin,cmax,3)
cbar.set_ticks(ticks)
cbar.ax.tick_params(labelsize=10)
if unitType == 'appConductivity':
cbar.set_label("App.Cond",size=12)
elif unitType == 'appResistivity':
cbar.set_label("App.Res.",size=12)
elif unitType == 'volt':
cbar.set_label("Potential (V)",size=12)
if not axlabel:
@@ -310,27 +307,24 @@ def plot_pseudoSection(DCsurvey, axs, stype='dpdp', dtype="appc", clim=None, cbl
return ph
def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
def gen_DCIPsurvey(endl, mesh, surveyType, AM_sep, MN_sep, nrx):
"""
Load in endpoints and survey specifications to generate Tx, Rx location
stations.
Load in endpoints and survey specifications to generate Tx, Rx location
stations.
Assumes flat topo for now...
Assumes flat topo for now...
Input:
:param endl -> input endpoints [x1, y1, z1, x2, y2, z2]
:object mesh -> SimPEG mesh object
:switch stype -> "dpdp" (dipole-dipole) | "pdp" (pole-dipole) | 'gradient'
: param a, n -> pole seperation, number of rx dipoles per tx
:param numpy.array endl: input endpoints [[x1, y1] , [x2, y2]]
:param Mesh mesh: SimPEG mesh object
:param string surveyType: 'dipole-dipole' | 'pole-dipole' | 'gradient'
:param float AM_sep: transmitter (A) - receiver (M) seperation
:param float b: receiver dipole seperation
:param float nrx: pole seperation, number of rx dipoles per tx
Output:
:param Tx, Rx -> List objects for each tx location
Lines: P1x, P1y, P1z, P2x, P2y, P2z
:rtype: DC.Survey, Src, Rx
:returns: DC survey, Source
Created on Wed December 9th, 2015
@author: dominiquef
!! Require clean up to deal with DCsurvey
!! Require clean up to deal with DCsurvey
"""
from SimPEG import np
@@ -346,17 +340,17 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
dl_x = ( endl[1,0] - endl[0,0] ) / dl_len
dl_y = ( endl[1,1] - endl[0,1] ) / dl_len
nstn = np.floor( dl_len / a )
nstn = np.floor( dl_len / AM_sep )
# Compute discrete pole location along line
stn_x = endl[0,0] + np.array(range(int(nstn)))*dl_x*a
stn_y = endl[0,1] + np.array(range(int(nstn)))*dl_y*a
stn_x = endl[0,0] + np.array(range(int(nstn)))*dl_x*AM_sep
stn_y = endl[0,1] + np.array(range(int(nstn)))*dl_y*AM_sep
# Create line of P1 locations
M = np.c_[stn_x, stn_y, np.ones(nstn).T*mesh.vectorNz[-1]]
# Create line of P2 locations
N = np.c_[stn_x+a*dl_x, stn_y+a*dl_y, np.ones(nstn).T*mesh.vectorNz[-1]]
N = np.c_[stn_x+AM_sep*dl_x, stn_y+AM_sep*dl_y, np.ones(nstn).T*mesh.vectorNz[-1]]
## Build list of Tx-Rx locations depending on survey type
# Dipole-dipole: Moving tx with [a] spacing -> [AB a MN1 a MN2 ... a MNn]
@@ -366,14 +360,14 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
SrcList = []
if stype != 'gradient':
if surveyType != 'gradient':
for ii in range(0, int(nstn)-1):
if stype == 'dpdp':
if surveyType == 'dipole-dipole':
tx = np.c_[M[ii,:],N[ii,:]]
elif stype == 'pdp':
elif surveyType == 'pole-dipole':
tx = np.c_[M[ii,:],M[ii,:]]
# Rx.append(np.c_[M[ii+1:indx,:],N[ii+1:indx,:]])
@@ -382,33 +376,33 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
AB = xy_2_r(tx[0,1],endl[1,0],tx[1,1],endl[1,1])
# Number of receivers to fit
nstn = np.min([np.floor( (AB - b) / a ) , n])
nstn = np.min([np.floor( (AB - MN_sep) / AM_sep ) , nrx])
# Check if there is enough space, else break the loop
if nstn <= 0:
continue
# Compute discrete pole location along line
stn_x = N[ii,0] + dl_x*b + np.array(range(int(nstn)))*dl_x*a
stn_y = N[ii,1] + dl_y*b + np.array(range(int(nstn)))*dl_y*a
stn_x = N[ii,0] + dl_x*MN_sep + np.array(range(int(nstn)))*dl_x*AM_sep
stn_y = N[ii,1] + dl_y*MN_sep + np.array(range(int(nstn)))*dl_y*AM_sep
# Create receiver poles
# Create line of P1 locations
P1 = np.c_[stn_x, stn_y, np.ones(nstn).T*mesh.vectorNz[-1]]
# Create line of P2 locations
P2 = np.c_[stn_x+a*dl_x, stn_y+a*dl_y, np.ones(nstn).T*mesh.vectorNz[-1]]
P2 = np.c_[stn_x+AM_sep*dl_x, stn_y+AM_sep*dl_y, np.ones(nstn).T*mesh.vectorNz[-1]]
Rx.append(np.c_[P1,P2])
rxClass = DC.RxDipole(P1, P2)
Tx.append(tx)
if stype == 'dpdp':
if surveyType == 'dipole-dipole':
srcClass = DC.SrcDipole([rxClass], M[ii,:],N[ii,:])
elif stype == 'pdp':
elif surveyType == 'pole-dipole':
srcClass = DC.SrcDipole([rxClass], M[ii,:],M[ii,:])
SrcList.append(srcClass)
elif stype == 'gradient':
elif surveyType == 'gradient':
# Gradient survey only requires Tx at end of line and creates a square
# grid of receivers at in the middle at a pre-set minimum distance
@@ -416,23 +410,23 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
Tx.append(np.c_[M[0,:],N[-1,:]])
# Get the edge limit of survey area
min_x = endl[0,0] + dl_x * b
min_y = endl[0,1] + dl_y * b
min_x = endl[0,0] + dl_x * MN_sep
min_y = endl[0,1] + dl_y * MN_sep
max_x = endl[1,0] - dl_x * b
max_y = endl[1,1] - dl_y * b
max_x = endl[1,0] - dl_x * MN_sep
max_y = endl[1,1] - dl_y * MN_sep
box_l = np.sqrt( (min_x - max_x)**2 + (min_y - max_y)**2 )
box_w = box_l/2.
nstn = np.floor( box_l / a )
nstn = np.floor( box_l / AM_sep )
# Compute discrete pole location along line
stn_x = min_x + np.array(range(int(nstn)))*dl_x*a
stn_y = min_y + np.array(range(int(nstn)))*dl_y*a
stn_x = min_x + np.array(range(int(nstn)))*dl_x*AM_sep
stn_y = min_y + np.array(range(int(nstn)))*dl_y*AM_sep
# Define number of cross lines
nlin = int(np.floor( box_w / a ))
nlin = int(np.floor( box_w / AM_sep ))
lind = range(-nlin,nlin+1)
ngrad = nstn * len(lind)
@@ -441,12 +435,12 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
for ii in range( len(lind) ):
# Move line in perpendicular direction by dipole spacing
lxx = stn_x - lind[ii]*a*dl_y
lyy = stn_y + lind[ii]*a*dl_x
lxx = stn_x - lind[ii]*AM_sep*dl_y
lyy = stn_y + lind[ii]*AM_sep*dl_x
M = np.c_[ lxx, lyy , np.ones(nstn).T*mesh.vectorNz[-1]]
N = np.c_[ lxx+a*dl_x, lyy+a*dl_y, np.ones(nstn).T*mesh.vectorNz[-1]]
N = np.c_[ lxx+AM_sep*dl_x, lyy+AM_sep*dl_y, np.ones(nstn).T*mesh.vectorNz[-1]]
rx[(ii*nstn):((ii+1)*nstn),:] = np.c_[M,N]
@@ -455,44 +449,38 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
srcClass = DC.SrcDipole([rxClass], M[0,:], N[-1,:])
SrcList.append(srcClass)
else:
print """stype must be either 'pdp', 'dpdp' or 'gradient'. """
print """surveyType must be either 'pole-dipole', 'dipole-dipole' or 'gradient'. """
survey = DC.SurveyDC(SrcList)
return survey, Tx, Rx
def writeUBC_DCobs(fileName, DCsurvey, dtype='3D', stype='SURFACE', iptype = 0):
def writeUBC_DCobs(fileName, DCsurvey, dim, surveyType, iptype = 0):
"""
Write UBC GIF DCIP 2D or 3D observation file
Input:
:string fileName -> including path where the file is written out
:DCsurvey DC survey class object
:string dtype -> either '2D' | '3D'
:string stype -> either 'SURFACE' | 'GENERAL'
Output:
:param UBC2D-Data file
:return
Last edit: February 16th, 2016
@author: dominiquef
:param string fileName: including path where the file is written out
:param Survey DCsurvey: DC survey class object
:param string dim: either '2D' | '3D'
:param string surveyType: either 'SURFACE' | 'GENERAL'
:rtype: file
:return: UBC2D-Data file
"""
from SimPEG import mkvc
assert (dtype=='2D') | (dtype=='3D'), "Data must be either '2D' | '3D'"
assert (stype=='SURFACE') | (stype=='GENERAL') | (stype=='SIMPLE'), "Data must be either 'SURFACE' | 'GENERAL' | 'SIMPLE'"
assert (dim=='2D') | (dim=='3D'), "Data must be either '2D' | '3D'"
assert (surveyType=='SURFACE') | (surveyType=='GENERAL') | (surveyType=='SIMPLE'), "Data must be either 'SURFACE' | 'GENERAL' | 'SIMPLE'"
fid = open(fileName,'w')
fid.write('! ' + surveyType + ' FORMAT\n')
if iptype!=0:
fid.write('IPTYPE=%i\n'%iptype)
else:
fid.write('! ' + stype + ' FORMAT\n')
count = 0
for ii in range(DCsurvey.nSrc):
@@ -506,33 +494,33 @@ def writeUBC_DCobs(fileName, DCsurvey, dtype='3D', stype='SURFACE', iptype = 0):
M = rx[0]
N = rx[1]
# Adapt source-receiver location for dtype and stype
if dtype=='2D':
# Adapt source-receiver location for dim and surveyType
if dim=='2D':
if stype == 'SIMPLE':
if surveyType == 'SIMPLE':
#fid.writelines("%e " % ii for ii in mkvc(tx[0,:]))
A = np.repeat(tx[0,0],M.shape[0],axis=0)
B = np.repeat(tx[0,1],M.shape[0],axis=0)
M = M[:,0]
N = N[:,0]
np.savetxt(fid, np.c_[A, B, M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%e',delimiter=' ',newline='\n')
else:
if stype == 'SURFACE':
if surveyType == 'SURFACE':
fid.writelines("%f " % ii for ii in mkvc(tx[0,:]))
M = M[:,0]
N = N[:,0]
if stype == 'GENERAL':
if surveyType == 'GENERAL':
# Flip sign for z-elevation to depth
tx[2::2,:] = -tx[2::2,:]
fid.writelines("%e " % ii for ii in mkvc(tx[::2,:]))
M = M[:,0::2]
N = N[:,0::2]
@@ -540,31 +528,31 @@ def writeUBC_DCobs(fileName, DCsurvey, dtype='3D', stype='SURFACE', iptype = 0):
# Flip sign for z-elevation to depth
M[:,1::2] = -M[:,1::2]
N[:,1::2] = -N[:,1::2]
fid.write('%i\n'% nD)
np.savetxt(fid, np.c_[ M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%f',delimiter=' ',newline='\n')
if dtype=='3D':
if dim=='3D':
if stype == 'SURFACE':
if surveyType == 'SURFACE':
fid.writelines("%e " % ii for ii in mkvc(tx[0:2,:]))
M = M[:,0:2]
N = N[:,0:2]
if stype == 'GENERAL':
if surveyType == 'GENERAL':
fid.writelines("%e " % ii for ii in mkvc(tx[0:3,:]))
fid.write('%i\n'% nD)
np.savetxt(fid, np.c_[ M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%e',delimiter=' ',newline='\n')
fid.write('\n')
count += nD
fid.close()
def convertObs_DC3D_to_2D(DCsurvey,lineID, flag = 'local'):
def convertObs_DC3D_to_2D(DCsurvey, lineID, flag='local'):
"""
Read DC survey and projects the coordinate system
according to the flag = 'Xloc' | 'Yloc' | 'local' (default)
@@ -573,15 +561,9 @@ def convertObs_DC3D_to_2D(DCsurvey,lineID, flag = 'local'):
The Z value is preserved, but Y coordinates zeroed.
Input:
:param survey3D
Output:
:figure survey2D
Edited April 6th, 2016
@author: dominiquef
:param DC.Survey survey3D: 3D simpeg DC survey
:rtype: DC.Survey
:return: survey2D
"""
from SimPEG import np
@@ -666,39 +648,34 @@ def convertObs_DC3D_to_2D(DCsurvey,lineID, flag = 'local'):
DCsurvey2D.std = np.asarray(DCsurvey.std)
return DCsurvey2D
def readUBC_DC3Dobs(fileName, dtype = 'DC'):
def readUBC_DC3Dobs(fileName, rtype = 'DC'):
"""
Read UBC GIF IP 3D observation file and generate survey
Input:
:param fileName, path to the UBC GIF 3D obs file
Output:
:param IPsurvey
:return
@author: dominiquef
:param string fileName:, path to the UBC GIF 3D obs file
:rtype: Survey
:return: DCIPsurvey
"""
zflag = True # Flag for z value provided
# Load file
if dtype == 'IP':
if rtype == 'IP':
obsfile = np.genfromtxt(fileName,delimiter=' \n',dtype=np.str,comments='IPTYPE')
elif dtype == 'DC':
elif rtype == 'DC':
obsfile = np.genfromtxt(fileName,delimiter=' \n',dtype=np.str,comments='!')
else:
print "dtype must be 'DC'(default) | 'IP'"
print "rtype must be 'DC'(default) | 'IP'"
# Pre-allocate
srcLists = []
Rx = []
d = []
wd = []
# Countdown for number of obs/tx
count = 0
@@ -717,7 +694,7 @@ def readUBC_DC3Dobs(fileName, dtype = 'DC'):
# Check if z value is provided, if False -> nan
if len(temp)==5:
tx = np.r_[temp[0:2],np.nan,temp[2:4],np.nan]
zflag = False # Pass on the flag to the receiver loc
else:
@@ -729,12 +706,12 @@ def readUBC_DC3Dobs(fileName, dtype = 'DC'):
temp = np.fromstring(obsfile[ii], dtype=float,sep=' ') # Get the string
# Filter out negative IP
# if temp[-2] < 0:
# if temp[-2] < 0:
# count = count -1
# print "Negative!"
#
#
# else:
# If the Z-location is provided, otherwise put nan
if zflag:
@@ -772,17 +749,9 @@ def readUBC_DC2Dobs(fileName):
------- NEEDS TO BE UPDATED ------
Read UBC GIF 2D observation file and generate arrays for tx-rx location
Input:
:param fileName, path to the UBC GIF 2D model file
Output:
:param rx, tx
:return
Created on Thu Nov 12 13:14:10 2015
@author: dominiquef
:param string fileName: path to the UBC GIF 2D model file
:rtype: (DC.Src, DC.Rx, ??, ??)
:return: source_locs, rx_locs, ??, ??
"""
from SimPEG import np
@@ -822,11 +791,9 @@ def readUBC_DC2Dpre(fileName):
Read UBC GIF DCIP 2D observation file and generate arrays for tx-rx location
Input:
:param fileName, path to the UBC GIF 3D obs file
Output:
DCsurvey
:return
:param string fileName: path to the UBC GIF 3D obs file
:rtype: DC.Survey
:return: DCsurvey
Created on Mon March 9th, 2016 << Doug's 70th Birthday !! >>
@@ -888,12 +855,9 @@ def readUBC_DC2DMesh(fileName):
"""
Read UBC GIF 2DTensor mesh and generate 2D Tensor mesh in simpeg
Input:
:param fileName, path to the UBC GIF mesh file
Output:
:param SimPEG TensorMesh 2D object
:return
:param string fileName: path to the UBC GIF mesh file
:rtype: Mesh.TensorMesh
:return: SimPEG TensorMesh 2D object
Created on Thu Nov 12 13:14:10 2015
@@ -959,12 +923,9 @@ def xy_2_lineID(DCsurvey):
they were collected. May need to generalize for random
point locations, but will be more expensive
Input:
:param DCdict Vectors of station location
Output:
:param LineID Vector of integers
:return
:param numpy.array DCdict: Vectors of station location
:rtype: numpy.array
:return: LineID Vector of integers
Created on Thu Feb 11, 2015
+3 -8
View File
@@ -169,9 +169,7 @@ class BaseEMProblem(Problem.BaseProblem):
dMeSigmaI_dI = -self.MeSigmaI**2
dMe_dsig = self.mesh.getEdgeInnerProductDeriv(self.curModel.sigma)(u)
dsig_dm = self.curModel.sigmaDeriv
return dMeSigmaI_dI * ( dMe_dsig * ( dsig_dm))
# return self.mesh.getEdgeInnerProductDeriv(self.curModel.sigma, invMat=True)(u)
return dMeSigmaI_dI * ( dMe_dsig * self.curModel.sigmaDeriv )
@property
def MfRho(self):
@@ -187,8 +185,7 @@ class BaseEMProblem(Problem.BaseProblem):
"""
Derivative of :code:`MfRho` with respect to the model.
"""
return self.mesh.getFaceInnerProductDeriv(self.curModel.rho)(u) * (-Utils.sdiag(self.curModel.rho**2) * self.curModel.sigmaDeriv)
# self.curModel.rhoDeriv
return self.mesh.getFaceInnerProductDeriv(self.curModel.rho)(u) * self.curModel.rhoDeriv
@property
def MfRhoI(self):
@@ -208,9 +205,7 @@ class BaseEMProblem(Problem.BaseProblem):
dMfRhoI_dI = -self.MfRhoI**2
dMf_drho = self.mesh.getFaceInnerProductDeriv(self.curModel.rho)(u)
return dMfRhoI_dI * ( dMf_drho * (-Utils.sdiag(self.curModel.rho**2) * self.curModel.sigmaDeriv) )
# return self.mesh.getFaceInnerProductDeriv(self.curModel.rho, invMat=True)(u) * self.curModel.rhoDeriv
return dMfRhoI_dI * ( dMf_drho * self.curModel.rhoDeriv )
class BaseEMSurvey(Survey.BaseSurvey):
+3 -3
View File
@@ -257,7 +257,7 @@ class Fields3D_e(Fields):
"""
# assuming primary does not depend on the model
return Zero()
return src.ePrimaryDeriv(self.prob, v, adjoint) #Zero()
def _bPrimary(self, eSolution, srcList):
"""
@@ -600,8 +600,8 @@ class Fields3D_b(Fields):
if adjoint:
return self._MeSigmaIDeriv(w).T * v - self._MeSigmaI.T * s_eDeriv
return self._MeSigmaIDeriv(w) * v - self._MeSigmaI * s_eDeriv
return self._MeSigmaIDeriv(w).T * v - self._MeSigmaI.T * s_eDeriv + src.ePrimaryDeriv(self.prob, v, adjoint)
return self._MeSigmaIDeriv(w) * v - self._MeSigmaI * s_eDeriv + src.ePrimaryDeriv(self.prob, v, adjoint)
def _j(self, bSolution, srcList):
"""
+4 -4
View File
@@ -74,7 +74,8 @@ class BaseFDEMProblem(BaseEMProblem):
self.curModel = m
Jv = self.dataPair(self.survey)
# Jv = self.dataPair(self.survey)
Jv = []
for freq in self.survey.freqs:
A = self.getA(freq)
@@ -89,9 +90,9 @@ class BaseFDEMProblem(BaseEMProblem):
for rx in src.rxList:
df_dmFun = getattr(f, '_{0}Deriv'.format(rx.projField), None)
df_dm_v = df_dmFun(src, du_dm_v, v, adjoint=False)
Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v)
Jv.append(rx.evalDeriv(src, self.mesh, f, df_dm_v))
Ainv.clean()
return Utils.mkvc(Jv)
return np.hstack(Jv)
def Jtvec(self, m, v, f=None):
"""
@@ -166,7 +167,6 @@ class BaseFDEMProblem(BaseEMProblem):
for i, src in enumerate(Srcs):
smi, sei = src.eval(self)
#Why are you adding?
s_m[:,i] = s_m[:,i] + smi
s_e[:,i] = s_e[:,i] + sei
+199 -1
View File
@@ -60,6 +60,18 @@ class BaseSrc(Survey.BaseSrc):
return Zero()
return self._bPrimary
def bPrimaryDeriv(self, prob, v, adjoint=False):
"""
Derivative of the primary magnetic flux density
:param Problem prob: FDEM Problem
:param numpy.ndarray v: vector
:param bool adjoint: adjoint?
:rtype: numpy.ndarray
:return: primary magnetic flux density
"""
return Zero()
def hPrimary(self, prob):
"""
Primary magnetic field
@@ -72,6 +84,18 @@ class BaseSrc(Survey.BaseSrc):
return Zero()
return self._hPrimary
def hPrimaryDeriv(self, prob, v, adjoint=False):
"""
Derivative of the primary magnetic field
:param Problem prob: FDEM Problem
:param numpy.ndarray v: vector
:param bool adjoint: adjoint?
:rtype: numpy.ndarray
:return: primary magnetic flux density
"""
return Zero()
def ePrimary(self, prob):
"""
Primary electric field
@@ -84,6 +108,18 @@ class BaseSrc(Survey.BaseSrc):
return Zero()
return self._ePrimary
def ePrimaryDeriv(self, prob, v, adjoint=False):
"""
Derivative of the primary electric field
:param Problem prob: FDEM Problem
:param numpy.ndarray v: vector
:param bool adjoint: adjoint?
:rtype: numpy.ndarray
:return: primary magnetic flux density
"""
return Zero()
def jPrimary(self, prob):
"""
Primary current density
@@ -96,6 +132,18 @@ class BaseSrc(Survey.BaseSrc):
return Zero()
return self._jPrimary
def jPrimaryDeriv(self, prob, v, adjoint=False):
"""
Derivative of the primary current density
:param Problem prob: FDEM Problem
:param numpy.ndarray v: vector
:param bool adjoint: adjoint?
:rtype: numpy.ndarray
:return: primary magnetic flux density
"""
return Zero()
def s_m(self, prob):
"""
Magnetic source term
@@ -555,7 +603,7 @@ class CircularLoop(BaseSrc):
a = MagneticLoopVectorPotential(self.loc, gridY, 'y', moment=self.radius, mu=self.mu)
else:
srcfct = MagneticDipoleVectorPotential
srcfct = MagneticLoopVectorPotential
ax = srcfct(self.loc, gridX, 'x', self.radius, mu=self.mu)
ay = srcfct(self.loc, gridY, 'y', self.radius, mu=self.mu)
az = srcfct(self.loc, gridZ, 'z', self.radius, mu=self.mu)
@@ -614,5 +662,155 @@ class CircularLoop(BaseSrc):
return -C.T * (MMui_s * self.bPrimary(prob))
class PrimSecSigma(BaseSrc):
def __init__(self, rxList, freq, sigBack, ePrimary, **kwargs):
self.sigBack = sigBack
BaseSrc.__init__(self, rxList, freq=freq, _ePrimary=ePrimary, **kwargs)
def s_e(self, prob):
return (prob.MeSigma - prob.mesh.getEdgeInnerProduct(self.sigBack)) * self.ePrimary(prob)
def s_eDeriv(self, prob, v, adjoint=False):
if adjoint:
return prob.MeSigmaDeriv(self.ePrimary(prob)).T * v
return prob.MeSigmaDeriv(self.ePrimary(prob)) * v
class PrimSecMappedSigma(BaseSrc):
"""
Primary-Secondary Source in which a mapping is provided to put the current model
onto the primary mesh. This is solved on every model update.
There are a lot of layers to the derivatives here!
**Required**
:param list rxList: Receiver List
:param float freq: frequency
:param ProblemFDEM primaryProblem: FDEM primary problem
:param SurveyFDEM primarySurvey: FDEM primary survey
**Optional**
:param Mapping map2meshSecondary: mapping current model to act as primary model on the secondary mesh
"""
def __init__(self, rxList, freq, primaryProblem, primarySurvey, map2meshSecondary = None ,**kwargs):
self.primaryProblem = primaryProblem
self.primarySurvey = primarySurvey
if self.primaryProblem.ispaired is False:
self.primaryProblem.pair(self.primarySurvey)
self.map2meshSecondary = map2meshSecondary
BaseSrc.__init__(self, rxList, freq=freq, **kwargs)
def _ProjPrimary(self, prob):
# if getattr(self, '__ProjPrimary', None) is None:
return self.primaryProblem.mesh.getInterpolationMatCartMesh(prob.mesh, locType='F', locTypeTo='E')
# return self.__ProjPrimary
def _primaryFields(self, prob, fieldType=None):
# TODO: cache and check if prob.curModel has changed
fields = self.primaryProblem.fields(prob.curModel.sigmaModel)
if fieldType is not None:
return fields[:,fieldType]
return fields
def _primaryFieldsDeriv(self, prob, v, adjoint=False, f=None):
if adjoint:
raise NotImplementedError
# TODO: this should not be hard-coded for j
# jp = self._primaryFields(prob)[:,'j']
# TODO: pull apart Jvec so that don't have to copy paste this code in
# A = self.primaryProblem.getA(self.freq)
# Ainv = self.primaryProblem.Solver(A, **self.primaryProblem.solverOpts) # create the concept of Ainv (actually a solve)
if f is None:
f = self._primaryFields(prob.curModel.sigmaModel)
freq = self.freq
A = self.primaryProblem.getA(freq)
Ainv = self.primaryProblem.Solver(A, **self.primaryProblem.solverOpts) # create the concept of Ainv (actually a solve)
src = self.primarySurvey.srcList[0]
# for src in self.survey.getSrcByFreq(freq):
u_src = Utils.mkvc(f[src, self.primaryProblem._solutionType])
dA_dm_v = self.primaryProblem.getADeriv(freq, u_src, v)
dRHS_dm_v = self.primaryProblem.getRHSDeriv(freq, src, v)
du_dm_v = Ainv * ( - dA_dm_v + dRHS_dm_v )
df_dmFun = getattr(f, '_{0}Deriv'.format('j'), None)
df_dm_v = df_dmFun(src, du_dm_v, v, adjoint=False)
# Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v)
Ainv.clean()
return df_dm_v
# return self.primaryProblem.Jvec(prob.curModel, v, f=f)
def ePrimary(self, prob, f=None):
if f is None:
f = self._primaryFields(prob)
ep = self._ProjPrimary(prob) * (
self.primaryProblem.MfI * (
self.primaryProblem.MfRho * f[:,'j'])
)
return Utils.mkvc(ep)
def ePrimaryDeriv(self, prob, v, adjoint=False, f=None):
if adjoint is True:
raise NotImplementedError
if f is None:
f = self._primaryFields(prob)
epDeriv = self._ProjPrimary(prob) * (
self.primaryProblem.MfI * (
(self.primaryProblem.MfRhoDeriv(f[:,'j']) * v)
+
(self.primaryProblem.MfRho * self._primaryFieldsDeriv(prob, v, f=f))
)
)
return Utils.mkvc(epDeriv)
def s_e(self, prob):
sigmaPrimary = self.map2meshSecondary * prob.curModel.sigmaModel
return Utils.mkvc((prob.MeSigma - prob.mesh.getEdgeInnerProduct(sigmaPrimary)) * self.ePrimary(prob))
def s_eDeriv(self, prob, v, adjoint=False):
if adjoint:
raise NotImplementedError
return prob.MeSigmaDeriv(self.ePrimary(prob)).T * v
sigmaPrimary = self.map2meshSecondary * prob.curModel.sigmaModel
sigmaPrimaryDeriv = self.map2meshSecondary.deriv(prob.curModel.sigmaModel)
f = self._primaryFields(prob)
ePrimary = self.ePrimary(prob,f=f)
return (prob.MeSigmaDeriv(ePrimary) * v
- prob.mesh.getEdgeInnerProductDeriv(sigmaPrimary)(ePrimary) * sigmaPrimaryDeriv * v
+ (prob.MeSigma - prob.mesh.getEdgeInnerProduct(sigmaPrimary)) * self.ePrimaryDeriv(prob, v, None, f=f)
)
+5 -7
View File
@@ -35,10 +35,9 @@ class BaseDCProblem(BaseEMProblem):
self.curModel = m
# Jv = self.dataPair(self.survey) #same size as the data
A = self.getA()
Jv = self.dataPair(self.survey) #same size as the data
Jv = []
A = self.getA()
for src in self.survey.srcList:
u_src = f[src, self._solutionType] # solution vector
@@ -49,10 +48,8 @@ class BaseDCProblem(BaseEMProblem):
for rx in src.rxList:
df_dmFun = getattr(f, '_%sDeriv'%rx.projField, None)
df_dm_v = df_dmFun(src, du_dm_v, v, adjoint=False)
# Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v)
Jv.append(rx.evalDeriv(src, self.mesh, f, df_dm_v))
# return Utils.mkvc(Jv)
return np.hstack(Jv)
Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v)
return Utils.mkvc(Jv)
def Jtvec(self, m, v, f=None):
if f is None:
@@ -67,6 +64,7 @@ class BaseDCProblem(BaseEMProblem):
Jtv = np.zeros(m.size)
AT = self.getA()
for src in self.survey.srcList:
u_src = f[src, self._solutionType]
for rx in src.rxList:
+8 -1
View File
@@ -43,7 +43,14 @@ class BaseRx(SimPEG.Survey.BaseRx):
elif adjoint:
return P.T*v
# DC.Rx.Dipole(locs)
# DC.Rx.Pole(locs)
class Pole(BaseRx):
def __init__(self, locs, rxType = 'phi', **kwargs):
BaseRx.__init__(self, locs, rxType)
# DC.Rx.Dipole(locsM, locsN)
class Dipole(BaseRx):
def __init__(self, locsM, locsN, rxType = 'phi', **kwargs):
+4 -8
View File
@@ -45,8 +45,7 @@ class BaseIPProblem(BaseEMProblem):
self.curModel = m
# Jv = self.dataPair(self.survey) #same size as the data
Jv = []
Jv = self.dataPair(self.survey) #same size as the data
A = self.getA()
@@ -59,16 +58,13 @@ class BaseIPProblem(BaseEMProblem):
for rx in src.rxList:
df_dmFun = getattr(f, '_%sDeriv'%rx.projField, None)
df_dm_v = df_dmFun(src, du_dm_v, v, adjoint=False)
# Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v)
Jv.append(rx.evalDeriv(src, self.mesh, f, df_dm_v))
Jv[src, rx] = rx.evalDeriv(src, self.mesh, f, df_dm_v)
# Conductivity (d u / d log sigma)
if self._formulation is 'EB':
# return -Utils.mkvc(Jv)
return -np.hstack(Jv)
return -Utils.mkvc(Jv)
# Conductivity (d u / d log rho)
if self._formulation is 'HJ':
# return Utils.mkvc(Jv)
return np.hstack(Jv)
return Utils.mkvc(Jv)
def Jtvec(self, m, v, f=None):
if f is None:
-104
View File
@@ -315,107 +315,3 @@ def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
return SrcList
def writeUBC_DCobs(fileName, DCsurvey, dtype='3D', stype='SURFACE', iptype = 0):
"""
Write UBC GIF DCIP 2D or 3D observation file
Input:
:string fileName -> including path where the file is written out
:DCsurvey DC survey class object
:string dtype -> either '2D' | '3D'
:string stype -> either 'SURFACE' | 'GENERAL'
Output:
:param UBC2D-Data file
:return
Last edit: February 16th, 2016
@author: dominiquef
"""
from SimPEG import mkvc
assert (dtype=='2D') | (dtype=='3D'), "Data must be either '2D' | '3D'"
assert (stype=='SURFACE') | (stype=='GENERAL') | (stype=='SIMPLE'), "Data must be either 'SURFACE' | 'GENERAL' | 'SIMPLE'"
fid = open(fileName,'w')
if iptype!=0:
fid.write('IPTYPE=%i\n'%iptype)
else:
fid.write('! ' + stype + ' FORMAT\n')
count = 0
for ii in range(DCsurvey.nSrc):
tx = np.c_[DCsurvey.srcList[ii].loc]
rx = DCsurvey.srcList[ii].rxList[0].locs
nD = DCsurvey.srcList[ii].nD
M = rx[0]
N = rx[1]
# Adapt source-receiver location for dtype and stype
if dtype=='2D':
if stype == 'SIMPLE':
#fid.writelines("%e " % ii for ii in mkvc(tx[0,:]))
A = np.repeat(tx[0,0],M.shape[0],axis=0)
B = np.repeat(tx[0,1],M.shape[0],axis=0)
M = M[:,0]
N = N[:,0]
np.savetxt(fid, np.c_[A, B, M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%e',delimiter=' ',newline='\n')
else:
if stype == 'SURFACE':
fid.writelines("%f " % ii for ii in mkvc(tx[0,:]))
M = M[:,0]
N = N[:,0]
if stype == 'GENERAL':
# Flip sign for z-elevation to depth
tx[2::2,:] = -tx[2::2,:]
fid.writelines("%e " % ii for ii in mkvc(tx[::2,:]))
M = M[:,0::2]
N = N[:,0::2]
# Flip sign for z-elevation to depth
M[:,1::2] = -M[:,1::2]
N[:,1::2] = -N[:,1::2]
fid.write('%i\n'% nD)
np.savetxt(fid, np.c_[ M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%f',delimiter=' ',newline='\n')
if dtype=='3D':
if stype == 'SURFACE':
fid.writelines("%e " % ii for ii in mkvc(tx[0:2,:]))
M = M[:,0:2]
N = N[:,0:2]
if stype == 'GENERAL':
fid.writelines("%e " % ii for ii in mkvc(tx[0:3,:]))
fid.write('%i\n'% nD)
np.savetxt(fid, np.c_[ M, N , DCsurvey.dobs[count:count+nD], DCsurvey.std[count:count+nD] ], fmt='%e',delimiter=' ',newline='\n')
fid.write('\n')
count += nD
fid.close()
+15 -17
View File
@@ -2,7 +2,7 @@ from SimPEG import Mesh, Utils, np, sp
import SimPEG.DCIP as DC
import time
def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', plotIt=True):
def run(loc=None, sig=None, radi=None, param=None, surveyType='dipole-dipole', unitType='appConductivity', plotIt=True):
"""
DC Forward Simulation
=====================
@@ -15,14 +15,14 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', p
loc = Location of spheres [[x1,y1,z1],[x2,y2,z2]]
radi = Radius of spheres [r1,r2]
param = Conductivity of background and two spheres [m0,m1,m2]
stype = survey type "pdp" (pole dipole) or "dpdp" (dipole dipole)
dtype = Data type "appr" (app res) | "appc" (app cond) | "volt" (potential)
surveyType = survey type 'pole-dipole' or 'dipole-dipole'
unitType = Data type "appResistivity" | "appConductivity" | "volt"
Created by @fourndo
"""
assert stype in ['pdp', 'dpdp'], "Source type (stype) must be pdp or dpdp (pole dipole or dipole dipole)"
assert dtype in ['appr', 'appc', 'volt'], "Data type (dtype) must be appr (app res) or appc (app cond) or volt (potential)"
assert surveyType in ['pole-dipole', 'dipole-dipole'], "Source type (surveyType) must be pdp or dpdp (pole dipole or dipole dipole)"
assert unitType in ['appResistivity', 'appConductivity', 'volt'], "Unit type (unitType) must be appResistivity or appConductivity or volt (potential)"
if loc is None:
loc = np.c_[[-50.,0.,-50.],[50.,0.,-50.]]
@@ -73,8 +73,8 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', p
locs = np.c_[mesh.gridCC[indx,0],mesh.gridCC[indx,1],np.ones(2).T*mesh.vectorNz[-1]]
# We will handle the geometry of the survey for you and create all the combination of tx-rx along line
# [Tx, Rx] = DC.gen_DCIPsurvey(locs, mesh, stype, param[0], param[1], param[2])
survey, Tx, Rx = DC.gen_DCIPsurvey(locs, mesh, stype, param[0], param[1], param[2])
# [Tx, Rx] = DC.gen_DCIPsurvey(locs, mesh, surveyType, param[0], param[1], param[2])
survey, Tx, Rx = DC.gen_DCIPsurvey(locs, mesh, surveyType, param[0], param[1], param[2])
# Define some global geometry
dl_len = np.sqrt( np.sum((locs[0,:] - locs[1,:])**2) )
@@ -118,8 +118,8 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', p
rxloc_N = np.asarray(Rx[ii][:,3:])
# For usual cases "dpdp" or "gradient"
if stype == 'pdp':
# For usual cases 'dipole-dipole' or "gradient"
if surveyType == 'pole-dipole':
# Create an "inifinity" pole
tx = np.squeeze(Tx[ii][:,0:1])
tinf = tx + np.array([dl_x,dl_y,0])*dl_len*2
@@ -157,12 +157,12 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', p
fig = plt.figure(figsize=(7,7))
ax = plt.subplot(2,1,1, aspect='equal')
# Plot the location of the spheres for reference
circle1=plt.Circle((loc[0,0],loc[2,0]),radi[0],color='w',fill=False, lw=3)
circle2=plt.Circle((loc[0,1],loc[2,1]),radi[1],color='k',fill=False, lw=3)
circle1=plt.Circle((loc[0,0], loc[2,0]), radi[0], color='w', fill=False, lw=3)
circle2=plt.Circle((loc[0,1], loc[2,1]), radi[1], color='k', fill=False, lw=3)
ax.add_artist(circle1)
ax.add_artist(circle2)
dat = mesh.plotSlice(np.log10(model), ax =ax, normal = 'Y',
dat = mesh.plotSlice(np.log10(model), ax = ax, normal = 'Y',
ind = indy,grid=True, clim = np.log10([sig.min(),sig.max()]))
ax.set_title('3-D model')
@@ -188,15 +188,13 @@ def run(loc=None, sig=None, radi=None, param=None, stype='dpdp', dtype='appc', p
ax2 = plt.subplot(2,1,2, aspect='equal')
# Plot the location of the spheres for reference
circle1=plt.Circle((loc[0,0],loc[2,0]),radi[0],color='w',fill=False, lw=3)
circle2=plt.Circle((loc[0,1],loc[2,1]),radi[1],color='k',fill=False, lw=3)
circle1=plt.Circle((loc[0,0], loc[2,0]), radi[0], color='w', fill=False, lw=3)
circle2=plt.Circle((loc[0,1], loc[2,1]), radi[1], color='k', fill=False, lw=3)
ax2.add_artist(circle1)
ax2.add_artist(circle2)
# Add the speudo section
dat = DC.plot_pseudoSection(survey2D,ax2,stype=stype, dtype = dtype)
# plt.scatter(Tx2d[0][:],Tx[0][2,:],s=40,c='g', marker='v')
dat = DC.plot_pseudoSection(survey2D, ax2, surveyType=surveyType, unitType=unitType) # plt.scatter(Tx2d[0][:],Tx[0][2,:],s=40,c='g', marker='v')
# plt.scatter(Rx2d[0][:],Rx[0][:,2::3],s=40,c='y')
# plt.plot(np.r_[Tx2d[0][0],Rx2d[-1][-1,-1]],np.ones(2)*mesh.vectorNz[-1], color='k')
ax2.set_title('Apparent Conductivity data')
+41
View File
@@ -0,0 +1,41 @@
from SimPEG import *
from SimPEG.Utils import surface2ind_topo
def run(plotIt=False, nx = 5, ny = 5):
"""
Here we show how to use :code:`Utils.surface2ind_topo` to identify cells below
a topographic surface.
"""
mesh = Mesh.TensorMesh([nx,ny], x0='CC') # 2D mesh
xtopo = np.linspace(mesh.gridN[:,0].min(), mesh.gridN[:,0].max())
topo = 0.4*np.sin(xtopo*5) # define a topographic surface
Topo = np.hstack([Utils.mkvc(xtopo,2),Utils.mkvc(topo,2)]) #make it an array
indcc = surface2ind_topo(mesh, Topo,'CC')
if plotIt:
from matplotlib.pylab import plt
from scipy.interpolate import interp1d
fig, ax = plt.subplots(1,1,figsize=(6,6))
mesh.plotGrid(ax=ax, nodes=True, centers=True)
ax.plot(xtopo,topo,'k',linewidth=1)
# ax.plot(mesh.vectorNx, interp1d(xtopo,topo)(mesh.vectorNx),'--k',linewidth=3)
ax.plot(mesh.vectorCCx, interp1d(xtopo,topo)(mesh.vectorCCx),'--k',linewidth=3)
aveN2CC = Utils.sdiag(mesh.aveN2CC.T.sum(1))*mesh.aveN2CC.T
a = aveN2CC * indcc
a[a > 0] = 1.
a[a < 0.25] = np.nan
a = a.reshape(mesh.vnN, order='F')
masked_array = np.ma.array(a, mask=np.isnan(a))
ax.pcolor(mesh.vectorNx,mesh.vectorNy,masked_array.T, cmap = plt.cm.gray,alpha=0.2)
plt.show()
if __name__ == '__main__':
run(plotIt=True)
+2 -1
View File
@@ -20,8 +20,9 @@ import Mesh_QuadTree_HangingNodes
import Mesh_Tensor_Creation
import MT_1D_ForwardAndInversion
import MT_3D_Foward
import Utils_surface2ind_topo
__examples__ = ["DC_Analytic_Dipole", "DC_Forward_PseudoSection", "EM_FDEM_1D_Inversion", "EM_FDEM_Analytic_MagDipoleWholespace", "EM_Schenkel_Morrison_Casing", "EM_TDEM_1D_Inversion", "FLOW_Richards_1D_Celia1990", "Forward_BasicDirectCurrent", "Inversion_IRLS", "Inversion_Linear", "Mesh_Basic_PlotImage", "Mesh_Basic_Types", "Mesh_Operators_CahnHilliard", "Mesh_QuadTree_Creation", "Mesh_QuadTree_FaceDiv", "Mesh_QuadTree_HangingNodes", "Mesh_Tensor_Creation", "MT_1D_ForwardAndInversion", "MT_3D_Foward"]
__examples__ = ["DC_Analytic_Dipole", "DC_Forward_PseudoSection", "EM_FDEM_1D_Inversion", "EM_FDEM_Analytic_MagDipoleWholespace", "EM_Schenkel_Morrison_Casing", "EM_TDEM_1D_Inversion", "FLOW_Richards_1D_Celia1990", "Forward_BasicDirectCurrent", "Inversion_IRLS", "Inversion_Linear", "Mesh_Basic_PlotImage", "Mesh_Basic_Types", "Mesh_Operators_CahnHilliard", "Mesh_QuadTree_Creation", "Mesh_QuadTree_FaceDiv", "Mesh_QuadTree_HangingNodes", "Mesh_Tensor_Creation", "MT_1D_ForwardAndInversion", "MT_3D_Foward", "Utils_surface2ind_topo"]
##### AUTOIMPORTS #####
+777 -83
View File
@@ -1,3 +1,4 @@
from __future__ import division
import Utils, numpy as np, scipy.sparse as sp
from scipy.sparse.linalg import LinearOperator
from Tests import checkDerivative
@@ -5,6 +6,7 @@ from PropMaps import PropMap, Property
from numpy.polynomial import polynomial
from scipy.interpolate import UnivariateSpline
import warnings
from SimPEG.Utils import Zero
class IdentityMap(object):
"""
@@ -17,7 +19,7 @@ class IdentityMap(object):
Utils.setKwargs(self, **kwargs)
if nP is not None:
assert type(nP) in [int, long], ' Number of parameters must be an integer.'
assert type(nP) in [int, long, np.int64], ' Number of parameters must be an integer.'
self.mesh = mesh
self._nP = nP
@@ -129,7 +131,15 @@ class IdentityMap(object):
class ComboMap(IdentityMap):
"""Combination of various maps."""
"""
Combination of various maps.
The ComboMap holds the information for multiplying and combining
maps. It also uses the chain rule to create the derivative.
Remember, any time that you make your own combination of mappings
be sure to test that the derivative is correct.
"""
def __init__(self, maps, **kwargs):
IdentityMap.__init__(self, None, **kwargs)
@@ -178,6 +188,12 @@ class ComboMap(IdentityMap):
class ExpMap(IdentityMap):
"""
Electrical conductivity varies over many orders of magnitude, so it is a common
technique when solving the inverse problem to parameterize and optimize in terms
of log conductivity. This makes sense not only because it ensures all conductivities
will be positive, but because this is fundamentally the space where conductivity
lives (i.e. it varies logarithmically).
Changes the model into the physical property.
A common example of this is to invert for electrical conductivity
@@ -449,6 +465,32 @@ class Mesh2Mesh(IdentityMap):
"""
Takes a model on one mesh are translates it to another mesh.
.. plot::
from SimPEG import *
import matplotlib.pyplot as plt
M = Mesh.TensorMesh([100,100])
h1 = Utils.meshTensor([(6,7,-1.5),(6,10),(6,7,1.5)])
h1 = h1/h1.sum()
M2 = Mesh.TensorMesh([h1,h1])
V = Utils.ModelBuilder.randomModel(M.vnC, seed=79, its=50)
v = Utils.mkvc(V)
modh = Maps.Mesh2Mesh([M,M2])
modH = Maps.Mesh2Mesh([M2,M])
H = modH * v
h = modh * H
ax = plt.subplot(131)
M.plotImage(v, ax=ax)
ax.set_title('Fine Mesh (Original)')
ax = plt.subplot(132)
M2.plotImage(H,clim=[0,1],ax=ax)
ax.set_title('Course Mesh')
ax = plt.subplot(133)
M.plotImage(h,clim=[0,1],ax=ax)
ax.set_title('Fine Mesh (Interpolated)')
plt.show()
"""
def __init__(self, meshes, **kwargs):
@@ -501,11 +543,19 @@ class InjectActiveCells(IdentityMap):
self.indInactive = np.logical_not(indActive)
if Utils.isScalar(valInactive):
self.valInactive = np.ones(self.nC)*float(valInactive)
self.valInactive[self.indActive] = 0.
else:
self.valInactive = valInactive.copy()
self.valInactive[self.indActive] = 0
if len(valInactive) == sum(self.indInactive):
self.valInactive = np.zeros(nC)
self.valInactive[self.indInactive] = valInactive.copy()
else:
assert len(self.valInactive) == self.nC, 'valInactive must be the size of nC or nInactive'
self.valInactive = valInactive.copy()
if any(self.valInactive[self.indActive] != 0.):
warnings.warn('the inactive has non-zero values in the active set.')
inds = np.nonzero(self.indActive)[0]
# inds[self.indActive]
self.P = sp.csr_matrix((np.ones(inds.size),(inds, range(inds.size))), shape=(self.nC, self.nP))
@property
@@ -533,83 +583,6 @@ class ActiveCells(InjectActiveCells):
FutureWarning)
InjectActiveCells.__init__(self, mesh, indActive, valInactive, nC)
class InjectActiveCellsTopo(IdentityMap):
"""
Active model parameters. Extend for cells on topography to air cell (only works for tensor mesh)
"""
indActive = None #: Active Cells
valInactive = None #: Values of inactive Cells
nC = None #: Number of cells in the full model
def __init__(self, mesh, indActive, nC=None):
self.mesh = mesh
self.nC = nC or mesh.nC
if indActive.dtype is not bool:
z = np.zeros(self.nC,dtype=bool)
z[indActive] = True
indActive = z
self.indActive = indActive
self.indInactive = np.logical_not(indActive)
inds = np.nonzero(self.indActive)[0]
self.P = sp.csr_matrix((np.ones(inds.size),(inds, range(inds.size))), shape=(self.nC, self.nP))
@property
def shape(self):
return (self.nC, self.nP)
@property
def nP(self):
"""Number of parameters in the model."""
return self.indActive.sum()
def _transform(self, m):
val_temp = np.zeros(self.mesh.nC)
val_temp[self.indActive] = m
valInactive = np.zeros(self.mesh.nC)
#1D
if self.mesh.dim == 1:
z_temp = self.mesh.gridCC
val_temp[~self.indActive] = val_temp[np.argmax(z_temp[self.indActive])]
#2D
elif self.mesh.dim == 2:
act_temp = self.indActive.reshape((self.mesh.nCx, self.mesh.nCy), order = 'F')
val_temp = val_temp.reshape((self.mesh.nCx, self.mesh.nCy), order = 'F')
y_temp = self.mesh.gridCC[:,1].reshape((self.mesh.nCx, self.mesh.nCy), order = 'F')
for i in range(self.mesh.nCx):
act_tempx = act_temp[i,:] == 1
val_temp[i,~act_tempx] = val_temp[i,np.argmax(y_temp[i,act_tempx])]
valInactive[~self.indActive] = Utils.mkvc(val_temp)[~self.indActive]
#3D
elif self.mesh.dim == 3:
act_temp = self.indActive.reshape((self.mesh.nCx*self.mesh.nCy, self.mesh.nCz), order = 'F')
val_temp = val_temp.reshape((self.mesh.nCx*self.mesh.nCy, self.mesh.nCz), order = 'F')
z_temp = self.mesh.gridCC[:,2].reshape((self.mesh.nCx*self.mesh.nCy, self.mesh.nCz), order = 'F')
for i in range(self.mesh.nCx*self.mesh.nCy):
act_tempxy = act_temp[i,:] == 1
val_temp[i,~act_tempxy] = val_temp[i,np.argmax(z_temp[i,act_tempxy])]
valInactive[~self.indActive] = Utils.mkvc(val_temp)[~self.indActive]
self.valInactive = valInactive
return self.P*m + self.valInactive
def inverse(self, D):
return self.P.T*D
def deriv(self, m):
return self.P
class ActiveCellsTopo(InjectActiveCellsTopo):
def __init__(self, mesh, indActive, valInactive, nC=None):
warnings.warn(
"`ActiveCellsTopo` is deprecated and will be removed in future versions. Use `InjectActiveCellsTopo` instead",
FutureWarning)
InjectActiveCellsTopo.__init__(self, mesh, indActive, valInactive, nC)
class Weighting(IdentityMap):
"""
@@ -651,6 +624,37 @@ class Weighting(IdentityMap):
def deriv(self, m):
return self.P
class Projection(IdentityMap):
"""
A map to rearrange parameters
"""
def __init__(self, indTo, indFrom, shape, mesh=None, **kwargs):
assert len(indTo) == len(indFrom)
self.P = sp.csr_matrix((np.ones(len(indTo)), (indTo, indFrom)), shape=shape)
self._shape = shape
super(Projection, self).__init__(mesh, **kwargs)
@property
def shape(self):
return self._shape
@property
def nP(self):
"""Number of parameters in the model."""
return self.shape[1]
def _transform(self, m):
return self.P*m
def deriv(self, m):
return self.P
class ComplexMap(IdentityMap):
"""ComplexMap
@@ -693,13 +697,13 @@ class CircleMap(IdentityMap):
Parameterize the model space using a circle in a wholespace.
..math::
.. math::
\sigma(m) = \sigma_1 + (\sigma_2 - \sigma_1)\left(\\arctan\left(100*\sqrt{(\\vec{x}-x_0)^2 + (\\vec{y}-y_0)}-r\\right) \pi^{-1} + 0.5\\right)
Define the model as:
..math::
.. math::
m = [\sigma_1, \sigma_2, x_0, y_0, r]
@@ -1052,7 +1056,697 @@ class SplineMap(IdentityMap):
return sp.csr_matrix(np.c_[g1,g2,g3])
class ParametrizedLayer(IdentityMap):
"""
Parametrized Layer Space
m = [val_background, val_layer, layer_center, layer_thickness]
.. plot::
:include-source:
from SimPEG import Mesh, Maps, np
import matplotlib.pyplot as plt
fig, ax = plt.subplots(1,1,figsize=(2,3))
mesh = Mesh.TensorMesh([50,50],x0='CC')
mapping = Maps.ParametrizedLayer(mesh)
m = np.hstack(np.r_[1., 2., -0.1, 0.2])
rho = mapping._transform(m)
mesh.plotImage(rho, ax=ax)
**Required**
:param Mesh mesh: SimPEG Mesh, 2D or 3D
**Optional**
:param float slopeFact: arctan slope factor - divided by the minimum h spacing to give the slope of the arctan functions
:param float slope: slope of the arctan function
:param numpy.ndarray indActive: bool vector with
"""
slopeFact = 1e2 # will be scaled by the mesh.
slope = None
indActive = None
def __init__(self, mesh, **kwargs):
super(ParametrizedLayer, self).__init__(mesh, **kwargs)
if self.slope is None:
self.slope = self.slopeFact / np.hstack(self.mesh.h).min()
self.x = [self.mesh.gridCC[:,0] if self.indActive is None else self.mesh.gridCC[self.indActive,0]][0]
if self.mesh.dim > 1:
self.y = [self.mesh.gridCC[:,1] if self.indActive is None else self.mesh.gridCC[self.indActive,1]][0]
if self.mesh.dim > 2:
self.z = [self.mesh.gridCC[:,2] if self.indActive is None else self.mesh.gridCC[self.indActive,2]][0]
@property
def nP(self):
return 4
@property
def shape(self):
if self.indActive is not None:
return (sum(self.indActive), self.nP)
return (self.mesh.nC, self.nP)
def mDict(self, m):
return {
'val_background': m[0],
'val_layer': m[1],
'layer_center': m[2],
'layer_thickness': m[3],
}
def _atanfct(self, xyz, xyzi, slope):
return np.arctan(slope * (xyz - xyzi))/np.pi + 0.5
def _atanfctDeriv(self, xyz, xyzi, slope):
# d/dx(atan(x)) = 1/(1+x**2)
x = slope * (xyz - xyzi)
dx = - slope
return (1./(1 + x**2))/np.pi * dx
def _atanLayer(self, mDict):
if self.mesh.dim == 2:
z = self.y
elif self.mesh.dim == 3:
z = self.z
layer_bottom = mDict['layer_center'] - mDict['layer_thickness'] / 2.
layer_top = mDict['layer_center'] + mDict['layer_thickness'] / 2.
return self._atanfct(z, layer_bottom, self.slope)*self._atanfct(z, layer_top, -self.slope)
def _atanLayerDeriv_layer_center(self, mDict):
if self.mesh.dim == 2:
z = self.y
elif self.mesh.dim == 3:
z = self.z
layer_bottom = mDict['layer_center'] - mDict['layer_thickness'] / 2.
layer_top = mDict['layer_center'] + mDict['layer_thickness'] / 2.
return (self._atanfctDeriv(z, layer_bottom, self.slope)*self._atanfct(z, layer_top, -self.slope)
+ self._atanfct(z, layer_bottom, self.slope)*self._atanfctDeriv(z, layer_top, -self.slope))
def _atanLayerDeriv_layer_thickness(self, mDict):
if self.mesh.dim == 2:
z = self.y
elif self.mesh.dim == 3:
z = self.z
layer_bottom = mDict['layer_center'] - mDict['layer_thickness'] / 2.
layer_top = mDict['layer_center'] + mDict['layer_thickness'] / 2.
return (-0.5*self._atanfctDeriv(z, layer_bottom, self.slope)*self._atanfct(z, layer_top, -self.slope)
+ 0.5*self._atanfct(z, layer_bottom, self.slope)*self._atanfctDeriv(z, layer_top, -self.slope))
def layer_cont(self, mDict):
return mDict['val_background'] + (mDict['val_layer'] - mDict['val_background'])*self._atanLayer(mDict)
def _transform(self, m):
mDict = self.mDict(m)
return self.layer_cont(mDict)
def _deriv_val_background(self, mDict):
return np.ones_like(self.x) - self._atanLayer(mDict)
def _deriv_val_layer(self, mDict):
return self._atanLayer(mDict)
def _deriv_layer_center(self, mDict):
return (mDict['val_layer']-mDict['val_background'])*self._atanLayerDeriv_layer_center(mDict)
def _deriv_layer_thickness(self, mDict):
return (mDict['val_layer']-mDict['val_background'])*self._atanLayerDeriv_layer_thickness(mDict)
def deriv(self, m):
mDict = self.mDict(m)
return sp.csr_matrix(np.vstack([
self._deriv_val_background(mDict),
self._deriv_val_layer(mDict),
self._deriv_layer_center(mDict),
self._deriv_layer_thickness(mDict),
]).T)
class ParametrizedCasingAndLayer(ParametrizedLayer):
"""
Parametrized layered space with casing.
m = [val_background, val_layer, val_casing, val_insideCasing, layer_center, layer_thickness, casing_radius, casing_thickness, casing_bottom, casing_top]
"""
def __init__(self, mesh, **kwargs):
assert mesh._meshType == 'CYL', 'Parametrized Casing in a layer map only works for a cyl mesh.'
super(ParametrizedCasingAndLayer, self).__init__(mesh, **kwargs)
@property
def nP(self):
return 10
@property
def shape(self):
if self.indActive is not None:
return (sum(self.indActive), self.nP)
return (self.mesh.nC, self.nP)
def mDict(self, m):
#m = [val_background, val_layer, val_casing, val_insideCasing, layer_center, layer_thickness, casing_radius, casing_thickness, casing_bottom, casing_top]
return {
'val_background': m[0],
'val_layer': m[1],
'val_casing': m[2],
'val_insideCasing': m[3],
'layer_center': m[4],
'layer_thickness': m[5],
'casing_radius': m[6],
'casing_thickness': m[7],
'casing_bottom': m[8],
'casing_top': m[9]
}
def _atanCasingLength(self, mDict):
return (self._atanfct(self.z, mDict['casing_top'], -self.slope)
* self._atanfct(self.z, mDict['casing_bottom'], self.slope))
def _atanCasingLengthDeriv_casing_top(self, mDict):
return (self._atanfctDeriv(self.z, mDict['casing_top'], -self.slope)
* self._atanfct(self.z, mDict['casing_bottom'], self.slope))
def _atanCasingLengthDeriv_casing_bottom(self, mDict):
return (self._atanfct(self.z, mDict['casing_top'], -self.slope)
* self._atanfctDeriv(self.z, mDict['casing_bottom'], self.slope))
def _atanInsideCasing(self, mDict):
casing_a = mDict['casing_radius'] - 0.5*mDict['casing_thickness']
return (self._atanCasingLength(mDict)
* self._atanfct(self.x, casing_a, -self.slope))
def _atanInsideCasingDeriv_casing_radius(self, mDict):
casing_a = mDict['casing_radius'] - 0.5*mDict['casing_thickness']
return (self._atanCasingLength(mDict)
* self._atanfctDeriv(self.x, casing_a, -self.slope))
def _atanInsideCasingDeriv_casing_thickness(self, mDict):
casing_a = mDict['casing_radius'] - 0.5*mDict['casing_thickness']
return (self._atanCasingLength(mDict)
* - 0.5*self._atanfctDeriv(self.x, casing_a, -self.slope))
def _atanInsideCasingDeriv_casing_top(self, mDict):
casing_a = mDict['casing_radius'] - 0.5*mDict['casing_thickness']
return (self._atanCasingLengthDeriv_casing_top(mDict)
* self._atanfct(self.x, casing_a, -self.slope))
def _atanInsideCasingDeriv_casing_bottom(self, mDict):
casing_a = mDict['casing_radius'] - 0.5*mDict['casing_thickness']
return (self._atanCasingLengthDeriv_casing_bottom(mDict)
* self._atanfct(self.x, casing_a, -self.slope))
def _atanCasing(self, mDict):
casing_a, casing_b = mDict['casing_radius'] - 0.5*mDict['casing_thickness'], mDict['casing_radius'] + 0.5*mDict['casing_thickness']
return (self._atanCasingLength(mDict)
* self._atanfct(self.x, casing_a, self.slope)
* self._atanfct(self.x, casing_b, -self.slope))
def _atanCasingDeriv_casing_radius(self, mDict):
casing_a, casing_b = mDict['casing_radius'] - 0.5*mDict['casing_thickness'], mDict['casing_radius'] + 0.5*mDict['casing_thickness']
return (self._atanCasingLength(mDict) * (
self._atanfctDeriv(self.x, casing_a, self.slope)
* self._atanfct(self.x, casing_b, -self.slope)
+
self._atanfct(self.x, casing_a, self.slope)
* self._atanfctDeriv(self.x, casing_b, -self.slope)
))
def _atanCasingDeriv_casing_thickness(self, mDict):
casing_a, casing_b = mDict['casing_radius'] - 0.5*mDict['casing_thickness'], mDict['casing_radius'] + 0.5*mDict['casing_thickness']
return (self._atanCasingLength(mDict) * (
- 0.5*self._atanfctDeriv(self.x, casing_a, self.slope)
* 0.5*self._atanfct(self.x, casing_b, -self.slope)
+
- 0.5*self._atanfct(self.x, casing_a, self.slope)
* 0.5*self._atanfctDeriv(self.x, casing_b, -self.slope)
))
def _atanCasingDeriv_casing_bottom(self, mDict):
casing_a, casing_b = mDict['casing_radius'] - 0.5*mDict['casing_thickness'], mDict['casing_radius'] + 0.5*mDict['casing_thickness']
return (self._atanCasingLengthDeriv_casing_bottom(mDict)
* self._atanfct(self.x, casing_a, self.slope)
* self._atanfct(self.x, casing_b, -self.slope))
def _atanCasingDeriv_casing_top(self, mDict):
casing_a, casing_b = mDict['casing_radius'] - 0.5*mDict['casing_thickness'], mDict['casing_radius'] + 0.5*mDict['casing_thickness']
return (self._atanCasingLengthDeriv_casing_top(mDict)
* self._atanfct(self.x, casing_a, self.slope)
* self._atanfct(self.x, casing_b, -self.slope))
def layer_cont(self, mDict):
return mDict['val_background'] + (mDict['val_layer']-mDict['val_background']) * self._atanLayer(mDict) # contribution from the layered background
def _transform(self, m):
mDict = self.mDict(m)
# assemble the model
layer = self.layer_cont(mDict)
casing = (mDict['val_casing'] - layer) * self._atanCasing(mDict)
insideCasing = (mDict['val_insideCasing'] - layer) * self._atanInsideCasing(mDict)
return layer + casing + insideCasing
def _deriv_val_background(self, mDict):
d_layer_cont_dval_background = 1. - self._atanLayer(mDict) # contribution from the layered background
d_casing_cont_dval_background = -1. * d_layer_cont_dval_background * self._atanCasing(mDict)
d_insideCasing_cont_dval_background = -1. * d_layer_cont_dval_background * self._atanInsideCasing(mDict)
return d_layer_cont_dval_background + d_casing_cont_dval_background + d_insideCasing_cont_dval_background
def _deriv_val_layer(self, mDict):
d_layer_cont_dval_layer = self._atanLayer(mDict)
d_casing_cont_dval_layer = -1. * d_layer_cont_dval_layer * self._atanCasing(mDict)
d_insideCasing_cont_dval_layer = -1. * d_layer_cont_dval_layer * self._atanInsideCasing(mDict)
return d_layer_cont_dval_layer + d_casing_cont_dval_layer + d_insideCasing_cont_dval_layer
def _deriv_val_casing(self, mDict):
d_layer_cont_dval_casing = 0.
d_casing_cont_dval_casing = self._atanCasing(mDict)
d_insideCasing_cont_dval_casing = 0.
return d_layer_cont_dval_casing + d_casing_cont_dval_casing + d_insideCasing_cont_dval_casing
def _deriv_val_insideCasing(self, mDict):
d_layer_cont_dval_insideCasing = 0.
d_casing_cont_dval_insideCasing = 0.
d_insideCasing_cont_dval_insideCasing = self._atanInsideCasing(mDict)
return d_layer_cont_dval_insideCasing + d_casing_cont_dval_insideCasing + d_insideCasing_cont_dval_insideCasing
def _deriv_layer_center(self, mDict):
d_layer_cont_dlayer_center = (mDict['val_layer'] - mDict['val_background']) * self._atanLayerDeriv_layer_center(mDict)
d_casing_cont_dlayer_center = - d_layer_cont_dlayer_center * self._atanCasing(mDict)
d_insideCasing_cont_dlayer_center = - d_layer_cont_dlayer_center * self._atanInsideCasing(mDict)
return d_layer_cont_dlayer_center + d_casing_cont_dlayer_center + d_insideCasing_cont_dlayer_center
def _deriv_layer_thickness(self, mDict):
d_layer_cont_dlayer_thickness = (mDict['val_layer']-mDict['val_background']) * self._atanLayerDeriv_layer_thickness(mDict)
d_casing_cont_dlayer_thickness = - d_layer_cont_dlayer_thickness * self._atanCasing(mDict)
d_insideCasing_cont_dlayer_thickness = - d_layer_cont_dlayer_thickness * self._atanInsideCasing(mDict)
return d_layer_cont_dlayer_thickness + d_casing_cont_dlayer_thickness + d_insideCasing_cont_dlayer_thickness
def _deriv_casing_radius(self, mDict):
layer = self.layer_cont(mDict)
d_layer_cont_dcasing_radius = 0.
d_casing_cont_dcasing_radius = (mDict['val_casing'] - layer) * self._atanCasingDeriv_casing_radius(mDict)
d_insideCasing_cont_dcasing_radius = (mDict['val_insideCasing'] - layer) * self._atanInsideCasingDeriv_casing_radius(mDict)
return d_layer_cont_dcasing_radius + d_casing_cont_dcasing_radius + d_insideCasing_cont_dcasing_radius
def _deriv_casing_thickness(self, mDict):
d_layer_cont_dcasing_thickness = 0.
d_casing_cont_dcasing_thickness = (mDict['val_casing'] - self.layer_cont(mDict)) * self._atanCasingDeriv_casing_thickness(mDict)
d_insideCasing_cont_dcasing_thickness = (mDict['val_insideCasing'] - self.layer_cont(mDict)) * self._atanInsideCasingDeriv_casing_thickness(mDict)
return d_layer_cont_dcasing_thickness + d_casing_cont_dcasing_thickness + d_insideCasing_cont_dcasing_thickness
def _deriv_casing_bottom(self, mDict):
d_layer_cont_dcasing_bottom = 0.
d_casing_cont_dcasing_bottom = (mDict['val_casing'] - self.layer_cont(mDict)) * self._atanCasingDeriv_casing_bottom(mDict)
d_insideCasing_cont_dcasing_bottom = (mDict['val_insideCasing'] - self.layer_cont(mDict)) * self._atanInsideCasingDeriv_casing_bottom(mDict)
return d_layer_cont_dcasing_bottom + d_casing_cont_dcasing_bottom + d_insideCasing_cont_dcasing_bottom
def _deriv_casing_top(self, mDict):
d_layer_cont_dcasing_top = 0.
d_casing_cont_dcasing_top = (mDict['val_casing'] - self.layer_cont(mDict)) * self._atanCasingDeriv_casing_top(mDict)
d_insideCasing_cont_dcasing_top = (mDict['val_insideCasing'] - self.layer_cont(mDict)) * self._atanInsideCasingDeriv_casing_top(mDict)
return d_layer_cont_dcasing_top + d_casing_cont_dcasing_top + d_insideCasing_cont_dcasing_top
def deriv(self, m):
mDict = self.mDict(m)
return sp.csr_matrix(np.vstack([
self._deriv_val_background(mDict),
self._deriv_val_layer(mDict),
self._deriv_val_casing(mDict),
self._deriv_val_insideCasing(mDict),
self._deriv_layer_center(mDict),
self._deriv_layer_thickness(mDict),
self._deriv_casing_radius(mDict),
self._deriv_casing_thickness(mDict),
self._deriv_casing_bottom(mDict),
self._deriv_casing_top(mDict),
]).T)
class ParametrizedBlockInLayer(ParametrizedLayer):
"""
Parametrized Block in a Layered Space
For 2D:
m = [val_background, val_layer, val_block, layer_center, layer_thickness, block_x0, block_dx]
For 3D:
m = [val_background, val_layer, val_block, layer_center, layer_thickness, block_x0, block_y0, block_dx, block_dy]
.. plot::
:include-source:
from SimPEG import Mesh, Maps, np
import matplotlib.pyplot as plt
fig, ax = plt.subplots(1,1,figsize=(2,3))
mesh = Mesh.TensorMesh([50,50],x0='CC')
mapping = Maps.ParametrizedBlockInLayer(mesh)
m = np.hstack(np.r_[1., 2., 3., -0.1, 0.2, 0.3, 0.2])
rho = mapping._transform(m)
mesh.plotImage(rho, ax=ax)
**Required**
:param Mesh mesh: SimPEG Mesh, 2D or 3D
**Optional**
:param float slopeFact: arctan slope factor - divided by the minimum h spacing to give the slope of the arctan functions
:param float slope: slope of the arctan function
:param numpy.ndarray indActive: bool vector with
"""
def __init__(self, mesh, **kwargs):
super(ParametrizedBlockInLayer, self).__init__(mesh, **kwargs)
@property
def nP(self):
if self.mesh.dim == 2:
return 7
elif self.mesh.dim == 3:
return 9
@property
def shape(self):
if self.indActive is not None:
return (sum(self.indActive), self.nP)
return (self.mesh.nC, self.nP)
def _mDict2d(self, m):
return{
'val_background': m[0],
'val_layer': m[1],
'val_block': m[2],
'layer_center': m[3],
'layer_thickness': m[4],
'x0_block': m[5],
'dx_block': m[6]
}
def _mDict3d(self, m):
return{
'val_background': m[0],
'val_layer': m[1],
'val_block': m[2],
'layer_center': m[3],
'layer_thickness': m[4],
'x0_block': m[5],
'y0_block': m[6],
'dx_block': m[7],
'dy_block': m[8]
}
def mDict(self, m):
if self.mesh.dim == 2:
return self._mDict2d(m)
elif self.mesh.dim == 3:
return self._mDict3d(m)
def _atanBlock2d(self, mDict):
return (self._atanLayer(mDict)
* self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope))
def _atanBlock2dDeriv_layer_center(self, mDict):
return (self._atanLayerDeriv_layer_center(mDict)
* self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope))
def _atanBlock2dDeriv_layer_thickness(self, mDict):
return (self._atanLayerDeriv_layer_thickness(mDict)
* self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope))
def _atanBlock2dDeriv_x0(self, mDict):
return self._atanLayer(mDict) * (
(self._atanfctDeriv(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope))
+
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfctDeriv(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope))
)
def _atanBlock2dDeriv_dx(self, mDict):
return self._atanLayer(mDict) * (
(self._atanfctDeriv(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope) * -0.5
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope))
+
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfctDeriv(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope) * 0.5)
)
def _atanBlock3d(self, mDict):
return (self._atanLayer(mDict)
* self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
def _atanBlock3dDeriv_layer_center(self, mDict):
return (self._atanLayerDeriv_layer_center(mDict)
* self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
def _atanBlock3dDeriv_layer_thickness(self, mDict):
return (self._atanLayerDeriv_layer_thickness(mDict)
* self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
def _atanBlock3dDeriv_x0(self, mDict):
return self._atanLayer(mDict) * (
(self._atanfctDeriv(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
+
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfctDeriv(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
)
def _atanBlock3dDeriv_y0(self, mDict):
return self._atanLayer(mDict) * (
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfctDeriv(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
+
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfctDeriv(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
)
def _atanBlock3dDeriv_dx(self, mDict):
return self._atanLayer(mDict) * (
(self._atanfctDeriv(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope) * -0.5
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
+
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfctDeriv(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope) * 0.5
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
)
def _atanBlock3dDeriv_dy(self, mDict):
return self._atanLayer(mDict) * (
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfctDeriv(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope) * -0.5
* self._atanfct(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope))
+
(self._atanfct(self.x, mDict['x0_block'] - 0.5*mDict['dx_block'], self.slope)
* self._atanfct(self.x, mDict['x0_block'] + 0.5*mDict['dx_block'], -self.slope)
* self._atanfct(self.y, mDict['y0_block'] - 0.5*mDict['dy_block'], self.slope)
* self._atanfctDeriv(self.y, mDict['y0_block'] + 0.5*mDict['dy_block'], -self.slope) * 0.5)
)
def _transform2d(self, m):
mDict = self.mDict(m)
# assemble the model
layer_cont = mDict['val_background'] + (mDict['val_layer']-mDict['val_background'])*self._atanLayer(mDict) # contribution from the layered background
block_cont = (mDict['val_block']-layer_cont)*self._atanBlock2d(mDict) # perturbation due to the block
return layer_cont + block_cont
def _deriv2d_val_background(self, mDict):
d_layer_dval_background = np.ones_like(self.x) - self._atanLayer(mDict)
d_block_dval_background = (-d_layer_dval_background)*self._atanBlock2d(mDict)
return d_layer_dval_background + d_block_dval_background
def _deriv2d_val_layer(self, mDict):
d_layer_dval_layer = self._atanLayer(mDict)
d_block_dval_layer = (-d_layer_dval_layer)*self._atanBlock2d(mDict)
return d_layer_dval_layer + d_block_dval_layer
def _deriv2d_val_block(self, mDict):
d_layer_dval_block = 0.
d_block_dval_block = (1.-d_layer_dval_block)*self._atanBlock2d(mDict)
return d_layer_dval_block + d_block_dval_block
def _deriv2d_layer_center(self, mDict):
d_layer_dlayer_center = (mDict['val_layer']-mDict['val_background'])*self._atanLayerDeriv_layer_center(mDict)
d_block_dlayer_center = ((mDict['val_block']-self.layer_cont(mDict))*self._atanBlock2dDeriv_layer_center(mDict)
- d_layer_dlayer_center*self._atanBlock2d(mDict))
return d_layer_dlayer_center + d_block_dlayer_center
def _deriv2d_layer_thickness(self, mDict):
d_layer_dlayer_thickness = (mDict['val_layer']-mDict['val_background'])*self._atanLayerDeriv_layer_thickness(mDict)
d_block_dlayer_thickness = ((mDict['val_block']-self.layer_cont(mDict))*self._atanBlock2dDeriv_layer_thickness(mDict)
- d_layer_dlayer_thickness*self._atanBlock2d(mDict))
return d_layer_dlayer_thickness + d_block_dlayer_thickness
def _deriv2d_x0_block(self, mDict):
d_layer_dx0 = 0.
d_block_dx0 = (mDict['val_block']-self.layer_cont(mDict))*self._atanBlock2dDeriv_x0(mDict)
return d_layer_dx0 + d_block_dx0
def _deriv2d_dx_block(self, mDict):
d_layer_ddx = 0.
d_block_ddx = (mDict['val_block']-self.layer_cont(mDict))*self._atanBlock2dDeriv_dx(mDict)
return d_layer_ddx + d_block_ddx
def _deriv2d(self, m):
mDict = self.mDict(m)
return np.vstack([
self._deriv2d_val_background(mDict),
self._deriv2d_val_layer(mDict),
self._deriv2d_val_block(mDict),
self._deriv2d_layer_center(mDict),
self._deriv2d_layer_thickness(mDict),
self._deriv2d_x0_block(mDict),
self._deriv2d_dx_block(mDict)
]).T
def _transform3d(self, m):
# parse model
mDict = self.mDict(m)
# assemble the model
layer_cont = mDict['val_background'] + (mDict['val_layer']-mDict['val_background'])*self._atanLayer(mDict) # contribution from the layered background
block_cont = (mDict['val_block']-layer_cont)*self._atanBlock3d(mDict) # perturbation due to the block
return layer_cont + block_cont
def _deriv3d_val_background(self, mDict):
d_layer_dval_background = np.ones_like(self.x) - self._atanLayer(mDict)
d_block_dval_background = (-d_layer_dval_background)*self._atanBlock3d(mDict)
return d_layer_dval_background + d_block_dval_background
def _deriv3d_val_layer(self, mDict):
d_layer_dval_layer = self._atanLayer(mDict)
d_block_dval_layer = (-d_layer_dval_layer)*self._atanBlock3d(mDict)
return d_layer_dval_layer + d_block_dval_layer
def _deriv3d_val_block(self, mDict):
d_layer_dval_block = 0.
d_block_dval_block = (1.-d_layer_dval_block)*self._atanBlock3d(mDict)
return d_layer_dval_block + d_block_dval_block
def _deriv3d_layer_center(self, mDict):
d_layer_dlayer_center = (mDict['val_layer']-mDict['val_background'])*self._atanLayerDeriv_layer_center(mDict)
d_block_dlayer_center = ((mDict['val_block']-self.layer_cont(mDict))*self._atanBlock3dDeriv_layer_center(mDict)
- d_layer_dlayer_center*self._atanBlock3d(mDict))
return d_layer_dlayer_center + d_block_dlayer_center
def _deriv3d_layer_thickness(self, mDict):
d_layer_dlayer_thickness = (mDict['val_layer']-mDict['val_background'])*self._atanLayerDeriv_layer_thickness(mDict)
d_block_dlayer_thickness = ((mDict['val_block']-self.layer_cont(mDict))*self._atanBlock3dDeriv_layer_thickness(mDict)
- d_layer_dlayer_thickness*self._atanBlock3d(mDict))
return d_layer_dlayer_thickness + d_block_dlayer_thickness
def _deriv3d_x0_block(self, mDict):
d_layer_dx0 = 0.
d_block_dx0 = (mDict['val_block']-self.layer_cont(mDict))*self._atanBlock3dDeriv_x0(mDict)
return d_layer_dx0 + d_block_dx0
def _deriv3d_y0_block(self, mDict):
d_layer_dy0 = 0.
d_block_dy0 = (mDict['val_block']-self.layer_cont(mDict))*self._atanBlock3dDeriv_y0(mDict)
return d_layer_dy0 + d_block_dy0
def _deriv3d_dx_block(self, mDict):
d_layer_ddx = 0.
d_block_ddx = (mDict['val_block']-self.layer_cont(mDict))*self._atanBlock3dDeriv_dx(mDict)
return d_layer_ddx + d_block_ddx
def _deriv3d_dy_block(self, mDict):
d_layer_ddy = 0.
d_block_ddy = (mDict['val_block']-self.layer_cont(mDict))*self._atanBlock3dDeriv_dy(mDict)
return d_layer_ddy + d_block_ddy
def _deriv3d(self, m):
mDict = self.mDict(m)
return np.vstack([
self._deriv3d_val_background(mDict),
self._deriv3d_val_layer(mDict),
self._deriv3d_val_block(mDict),
self._deriv3d_layer_center(mDict),
self._deriv3d_layer_thickness(mDict),
self._deriv3d_x0_block(mDict),
self._deriv3d_y0_block(mDict),
self._deriv3d_dx_block(mDict),
self._deriv3d_dy_block(mDict),
]).T
def _transform(self, m):
if self.mesh.dim == 2:
return self._transform2d(m)
elif self.mesh.dim == 3:
return self._transform3d(m)
def deriv(self, m):
if self.mesh.dim == 2:
return sp.csr_matrix(self._deriv2d(m))
elif self.mesh.dim == 3:
return sp.csr_matrix(self._deriv3d(m))
+12 -23
View File
@@ -205,30 +205,19 @@ class TensorMeshIO(object):
:param simpeg.Mesh.TensorMesh mesh: The mesh
"""
if mesh.dim ==3:
s = ''
s += '%i %i %i\n' %tuple(mesh.vnC)
origin = mesh.x0 + np.array([0,0,mesh.hz.sum()]) # Have to it in the same operation or use mesh.x0.copy(), otherwise the mesh.x0 is updated.
origin.dtype = float
assert mesh.dim == 3
s = ''
s += '%i %i %i\n' %tuple(mesh.vnC)
origin = mesh.x0 + np.array([0,0,mesh.hz.sum()]) # Have to it in the same operation or use mesh.x0.copy(), otherwise the mesh.x0 is updated.
origin.dtype = float
s += '%.2f %.2f %.2f\n' %tuple(origin)
s += ('%.2f '*mesh.nCx+'\n')%tuple(mesh.hx)
s += ('%.2f '*mesh.nCy+'\n')%tuple(mesh.hy)
s += ('%.2f '*mesh.nCz+'\n')%tuple(mesh.hz[::-1])
f = open(fileName, 'w')
f.write(s)
f.close()
elif mesh.dim==2:
fid = open(fileName,'w')
fid.write('%i\n'% mesh.nCx)
fid.write('%f %f 1\n'% (mesh.vectorNx[0],mesh.vectorNx[1]))
np.savetxt(fid, np.c_[mesh.vectorNx[2:],np.ones(mesh.nCx-1)], fmt='\t %e %i',delimiter=' ',newline='\n')
fid.write('\n')
fid.write('%i\n'% mesh.nCy)
fid.write('%f %f 1\n'%( 0,mesh.hy[-1]))
np.savetxt(fid, np.c_[np.cumsum(mesh.hy[-2::-1])+mesh.hy[-1],np.ones(mesh.nCy-1)], fmt='\t %e %i',delimiter=' ',newline='\n')
fid.close()
s += '%.2f %.2f %.2f\n' %tuple(origin)
s += ('%.2f '*mesh.nCx+'\n')%tuple(mesh.hx)
s += ('%.2f '*mesh.nCy+'\n')%tuple(mesh.hy)
s += ('%.2f '*mesh.nCz+'\n')%tuple(mesh.hz[::-1])
f = open(fileName, 'w')
f.write(s)
f.close()
if models is None: return
assert type(models) is dict, 'models must be a dict'
+2 -2
View File
@@ -74,7 +74,7 @@ class Property(object):
if linkedMap is None:
return None
linkMap = linkMapClass(None) * linkedMap
m = getattr(self, '%s'%linkName)
m = getattr(self, '%sModel'%linkName)
return linkMap.deriv( m )
m = getattr(self, '%sModel'%prop.name)
@@ -239,7 +239,7 @@ class PropMap(object):
setattr(self, '%sMap'%name, mapping)
setattr(self, '%sIndex'%name, slices.get(name, slice(nP, nP + mapping.nP)))
nP += mapping.nP
self.nP = nP
self.nP = nP
@property
def defaultInvProp(self):
+13 -5
View File
@@ -39,7 +39,7 @@ class RegularizationMesh(object):
if self.indActive is None:
self._nC = self.mesh.nC
else:
self._nC = sum(self.indActive)
self._nC = int(sum(self.indActive))
return self._nC
@property
@@ -304,7 +304,7 @@ class BaseRegularization(object):
mesh = None #: A SimPEG.Mesh instance.
mref = None #: Reference model.
def __init__(self, mesh, mapping=None, indActive=None, **kwargs):
def __init__(self, mesh=None, nP=None, mapping=None, indActive=None, **kwargs):
Utils.setKwargs(self, **kwargs)
assert isinstance(mesh, Mesh.BaseMesh), "mesh must be a SimPEG.Mesh object."
if indActive is not None and indActive.dtype != 'bool':
@@ -314,11 +314,19 @@ class BaseRegularization(object):
if indActive is not None and mapping is None:
mapping = Maps.IdentityMap(nP=indActive.nonzero()[0].size)
if mesh is None and nP is None:
raise Exception, 'either Mesh or number of parameters must be provided to the BaseRegularization'
self.regmesh = RegularizationMesh(mesh,indActive)
self.mapping = mapping or self.mapPair(mesh)
self.mapping._assertMatchesPair(self.mapPair)
self.indActive = indActive
if mesh is not None and nP is None:
nP = self.regmesh.nC
self.nP = nP
self.mapping = mapping or self.mapPair(nP=self.nP)
self.mapping._assertMatchesPair(self.mapPair)
@property
def parent(self):
"""This is the parent of the regularization."""
@@ -346,7 +354,7 @@ class BaseRegularization(object):
@property
def W(self):
"""Full regularization weighting matrix W."""
return sp.identity(self.regmesh.nC)
return sp.identity(self.nP)
@Utils.timeIt
def eval(self, m):
+1
View File
@@ -7,3 +7,4 @@ from CounterUtils import *
import ModelBuilder
import SolverUtils
from coordutils import *
from modelutils import *
+63
View File
@@ -0,0 +1,63 @@
from matutils import mkvc, ndgrid
import numpy as np
def surface2ind_topo(mesh, topo, gridLoc='CC'):
# def genActiveindfromTopo(mesh, topo):
"""
Get active indices from topography
"""
if mesh.dim == 3:
from scipy.interpolate import NearestNDInterpolator
Ftopo = NearestNDInterpolator(topo[:,:2], topo[:,2])
if gridLoc == 'CC':
XY = ndgrid(mesh.vectorCCx, mesh.vectorCCy)
Zcc = mesh.gridCC[:,2].reshape((np.prod(mesh.vnC[:2]), mesh.nCz), order='F')
gridTopo = Ftopo(XY)
actind = [gridTopo[ixy] <= Zcc[ixy,:] for ixy in range(np.prod(mesh.vnC[0]))]
actind = np.hstack(actind)
elif gridLoc == 'N':
XY = ndgrid(mesh.vectorNx, mesh.vectorNy)
gridTopo = Ftopo(XY).reshape(mesh.vnN[:2], order='F')
if mesh._meshType not in ['TENSOR', 'CYL', 'BASETENSOR']:
raise NotImplementedError('Nodal surface2ind_topo not implemented for %s mesh'%mesh._meshType)
Nz = mesh.vectorNz[1:] # TODO: this will only work for tensor meshes
actind = np.array([False]*mesh.nC).reshape(mesh.vnC, order='F')
for ii in range(mesh.nCx):
for jj in range(mesh.nCy):
actind[ii,jj,:] = [np.all(gridTopo[ii:ii+2, jj:jj+2] >= Nz[kk]) for kk in range(len(Nz)) ]
elif mesh.dim == 2:
from scipy.interpolate import interp1d
Ftopo = interp1d(topo[:,0], topo[:,1])
if gridLoc == 'CC':
gridTopo = Ftopo(mesh.gridCC[:,0])
actind = mesh.gridCC[:,1] <= gridTopo
elif gridLoc == 'N':
gridTopo = Ftopo(mesh.vectorNx)
if mesh._meshType not in ['TENSOR', 'CYL', 'BASETENSOR']:
raise NotImplementedError('Nodal surface2ind_topo not implemented for %s mesh'%mesh._meshType)
Ny = mesh.vectorNy[1:] # TODO: this will only work for tensor meshes
actind = np.array([False]*mesh.nC).reshape(mesh.vnC, order='F')
for ii in range(mesh.nCx):
actind[ii,:] = [np.all(gridTopo[ii:ii+2] > Ny[kk]) for kk in range(len(Ny)) ]
else:
raise NotImplementedError('surface2ind_topo not implemented for 1D mesh')
return mkvc(actind)
+1 -83
View File
@@ -122,92 +122,10 @@ When these are used in the inverse problem, this is extremely important!!
The API
=======
.. autoclass:: SimPEG.Maps.IdentityMap
.. automodule:: SimPEG.Maps
:members:
:undoc-members:
Common Maps
===========
Exponential Map
---------------
Electrical conductivity varies over many orders of magnitude, so it is a common
technique when solving the inverse problem to parameterize and optimize in terms
of log conductivity. This makes sense not only because it ensures all conductivities
will be positive, but because this is fundamentally the space where conductivity
lives (i.e. it varies logarithmically).
.. autoclass:: SimPEG.Maps.ExpMap
:members:
:undoc-members:
Vertical 1D Map
---------------
.. autoclass:: SimPEG.Maps.Vertical1DMap
:members:
:undoc-members:
Map 2D Cross-Section to 3D Model
--------------------------------
.. autoclass:: SimPEG.Maps.Map2Dto3D
:members:
:undoc-members:
Mesh to Mesh Map
----------------
.. plot::
from SimPEG import *
import matplotlib.pyplot as plt
M = Mesh.TensorMesh([100,100])
h1 = Utils.meshTensor([(6,7,-1.5),(6,10),(6,7,1.5)])
h1 = h1/h1.sum()
M2 = Mesh.TensorMesh([h1,h1])
V = Utils.ModelBuilder.randomModel(M.vnC, seed=79, its=50)
v = Utils.mkvc(V)
modh = Maps.Mesh2Mesh([M,M2])
modH = Maps.Mesh2Mesh([M2,M])
H = modH * v
h = modh * H
ax = plt.subplot(131)
M.plotImage(v, ax=ax)
ax.set_title('Fine Mesh (Original)')
ax = plt.subplot(132)
M2.plotImage(H,clim=[0,1],ax=ax)
ax.set_title('Course Mesh')
ax = plt.subplot(133)
M.plotImage(h,clim=[0,1],ax=ax)
ax.set_title('Fine Mesh (Interpolated)')
plt.show()
.. autoclass:: SimPEG.Maps.Mesh2Mesh
:members:
:undoc-members:
Some Extras
===========
Combo Map
---------
The ComboMap holds the information for multiplying and combining
maps. It also uses the chain rule to create the derivative.
Remember, any time that you make your own combination of mappings
be sure to test that the derivative is correct.
.. autoclass:: SimPEG.Maps.ComboMap
:members:
:undoc-members:
+3 -2
View File
@@ -20,8 +20,9 @@ INPUT:
loc = Location of spheres [[x1,y1,z1],[x2,y2,z2]]
radi = Radius of spheres [r1,r2]
param = Conductivity of background and two spheres [m0,m1,m2]
stype = survey type "pdp" (pole dipole) or "dpdp" (dipole dipole)
dtype = Data type "appr" (app res) | "appc" (app cond) | "volt" (potential)
surveyType = survey type 'pole-dipole' or 'dipole-dipole'
unitType = Data type "appResistivity" | "appConductivity" | "volt"
Created by @fourndo
+24
View File
@@ -0,0 +1,24 @@
.. _examples_Utils_surface2ind_topo:
.. --------------------------------- ..
.. ..
.. THIS FILE IS AUTO GENEREATED ..
.. ..
.. SimPEG/Examples/__init__.py ..
.. ..
.. --------------------------------- ..
Here we show how to use :code:`Utils.surface2ind_topo` to identify cells below
a topographic surface.
.. plot::
from SimPEG import Examples
Examples.Utils_surface2ind_topo.run()
.. literalinclude:: ../../SimPEG/Examples/Utils_surface2ind_topo.py
:language: python
:linenos:
View File
+29
View File
@@ -1,6 +1,7 @@
import unittest
from SimPEG import *
from scipy.constants import mu_0
from SimPEG import Tests
class MyPropMap(Maps.PropMap):
@@ -187,6 +188,34 @@ class TestPropMaps(unittest.TestCase):
MyReciprocalPropMap([('sigma', iMap), ('mu', iMap)]) # This should be fine
def test_linked_derivs_sigma(self):
mesh = Mesh.TensorMesh([4,5], x0='CC')
mapping = Maps.ExpMap(mesh)
propmap = MyReciprocalPropMap([('rho', mapping)])
x0 = np.random.rand(mesh.nC)
m = propmap(x0)
# test Sigma
testme = lambda v: [1./(m.rhoMap*v), m.sigmaDeriv]
print 'Testing Rho from Sigma'
Tests.checkDerivative(testme, x0, dx=0.01*x0, num=5, plotIt=False)
def test_linked_derivs_rho(self):
mesh = Mesh.TensorMesh([4,5], x0='CC')
mapping = Maps.ExpMap(mesh)
propmap = MyReciprocalPropMap([('sigma', mapping)])
x0 = np.random.rand(mesh.nC)
m = propmap(x0)
# test Sigma
testme = lambda v: [1./(m.sigmaMap*v), m.rhoDeriv]
print 'Testing Rho from Sigma'
Tests.checkDerivative(testme, x0, dx=0.01*x0, num=5, plotIt=False)
if __name__ == '__main__':
unittest.main()
+15 -2
View File
@@ -5,8 +5,10 @@ from scipy.sparse.linalg import dsolve
TOL = 1e-14
MAPS_TO_TEST_2D = ["CircleMap", "ComplexMap", "ExpMap", "IdentityMap", "SurjectVertical1D", "Weighting", "SurjectFull","FullMap","Vertical1DMap"]
MAPS_TO_TEST_3D = [ "ComplexMap", "ExpMap", "IdentityMap", "SurjectVertical1D", "Weighting", "SurjectFull","FullMap","Vertical1DMap"]
MAPS_TO_TEST_2D = ["CircleMap", "ComplexMap", "ExpMap", "IdentityMap", "SurjectVertical1D", "Weighting", "SurjectFull", "FullMap", "Vertical1DMap", "ParametrizedLayer", "ParametrizedBlockInLayer"]
MAPS_TO_TEST_3D = [ "ComplexMap", "ExpMap", "IdentityMap", "SurjectVertical1D", "Weighting", "SurjectFull", "FullMap", "Vertical1DMap", "ParametrizedLayer", "ParametrizedBlockInLayer"]
MAPS_TO_TEST_CYL = [ "ComplexMap", "ExpMap", "IdentityMap", "SurjectVertical1D", "Weighting", "SurjectFull", "FullMap", "Vertical1DMap", "ParametrizedLayer"]
class MapTests(unittest.TestCase):
@@ -17,6 +19,8 @@ class MapTests(unittest.TestCase):
self.mesh2 = Mesh.TensorMesh([a, b], x0=np.array([3, 5]))
self.mesh3 = Mesh.TensorMesh([a, b, [3,4]], x0=np.array([3, 5, 2]))
self.mesh22 = Mesh.TensorMesh([b, a], x0=np.array([3, 5]))
self.meshCyl = Mesh.CylMesh([10.,1.,10.], x0='00C')
print self.meshCyl._meshType
def test_transforms2D(self):
for M in MAPS_TO_TEST_2D:
@@ -28,6 +32,15 @@ class MapTests(unittest.TestCase):
maps = getattr(Maps, M)(self.mesh3)
self.assertTrue(maps.test())
def test_transformsCyl(self):
for M in MAPS_TO_TEST_CYL:
maps = getattr(Maps, M)(self.meshCyl)
self.assertTrue(maps.test())
def test_ParametricCasingAndLayer(self):
mapping = Maps.ParametrizedCasingAndLayer(self.meshCyl)
m = np.r_[-2., 1., 6., 2., -0.1, 0.2, 0.5, 0.2, -0.2, 0.2]
self.assertTrue(mapping.test(m))
def test_transforms_logMap_reciprocalMap(self):
# Note that log/reciprocal maps can be kinda finicky, so we are being explicit about the random seed.