def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
"""
Load in endpoints and survey specifications to generate Tx, Rx location
stations.
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
Output:
:param Tx, Rx -> List objects for each tx location
Lines: P1x, P1y, P1z, P2x, P2y, P2z
Created on Wed December 9th, 2015
@author: dominiquef
!! Require clean up to deal with DCsurvey
"""
from SimPEG import np
def xy_2_r(x1, x2, y1, y2):
r = np.sqrt(np.sum((x2 - x1)**2 + (y2 - y1)**2))
return r
## Evenly distribute electrodes and put on surface
# Mesure survey length and direction
dl_len = xy_2_r(endl[0, 0], endl[1, 0], endl[0, 1], endl[1, 1])
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)
# 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
if mesh.dim == 2:
ztop = mesh.vectorNy[-1]
# Create line of P1 locations
M = np.c_[stn_x, np.ones(nstn).T * ztop]
# Create line of P2 locations
N = np.c_[stn_x + a * dl_x, np.ones(nstn).T * ztop]
elif mesh.dim == 3:
ztop = mesh.vectorNz[-1]
# Create line of P1 locations
M = np.c_[stn_x, stn_y, np.ones(nstn).T * ztop]
# Create line of P2 locations
N = np.c_[stn_x + a * dl_x, stn_y + a * dl_y, np.ones(nstn).T * ztop]
## Build list of Tx-Rx locations depending on survey type
# Dipole-dipole: Moving tx with [a] spacing -> [AB a MN1 a MN2 ... a MNn]
# Pole-dipole: Moving pole on one end -> [A a MN1 a MN2 ... MNn a B]
SrcList = []
if stype != 'gradient':
for ii in range(0, int(nstn) - 1):
if stype == 'dipole-dipole':
tx = np.c_[M[ii, :], N[ii, :]]
elif stype == 'pole-dipole':
tx = np.c_[M[ii, :], M[ii, :]]
else:
raise Exception(
'The stype must be "dipole-dipole" or "pole-dipole"')
# Rx.append(np.c_[M[ii+1:indx,:],N[ii+1:indx,:]])
# Current elctrode seperation
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])
# 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
# Create receiver poles
if mesh.dim == 3:
# Create line of P1 locations
P1 = np.c_[stn_x, stn_y, np.ones(nstn).T * ztop]
# Create line of P2 locations
P2 = np.c_[stn_x + a * dl_x, stn_y + a * dl_y,
np.ones(nstn).T * ztop]
rxClass = DC.Rx.Dipole(P1, P2)
elif mesh.dim == 2:
# Create line of P1 locations
P1 = np.c_[stn_x, np.ones(nstn).T * ztop]
# Create line of P2 locations
P2 = np.c_[stn_x + a * dl_x, np.ones(nstn).T * ztop]
rxClass = DC.Rx.Dipole_ky(P1, P2)
if stype == 'dipole-dipole':
srcClass = DC.Src.Dipole([rxClass], M[ii, :], N[ii, :])
elif stype == 'pole-dipole':
srcClass = DC.Src.Pole([rxClass], M[ii, :])
SrcList.append(srcClass)
elif stype == '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
# Get the edge limit of survey area
min_x = endl[0, 0] + dl_x * b
min_y = endl[0, 1] + dl_y * b
max_x = endl[1, 0] - dl_x * b
max_y = endl[1, 1] - dl_y * b
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)
# 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
# Define number of cross lines
nlin = int(np.floor(box_w / a))
lind = range(-nlin, nlin + 1)
ngrad = nstn * len(lind)
rx = np.zeros([ngrad, 6])
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
M = np.c_[lxx, lyy, np.ones(nstn).T * ztop]
N = np.c_[lxx + a * dl_x, lyy + a * dl_y, np.ones(nstn).T * ztop]
rx[(ii * nstn):((ii + 1) * nstn), :] = np.c_[M, N]
if mesh.dim == 3:
rxClass = DC.Rx.Dipole(rx[:, :3], rx[:, 3:])
elif mesh.dim == 2:
M = M[:, [0, 2]]
N = N[:, [0, 2]]
rxClass = DC.Rx.Dipole_ky(rx[:, [0, 2]], rx[:, [3, 5]])
srcClass = DC.Src.Dipole([rxClass], M[0, :], N[-1, :])
SrcList.append(srcClass)
else:
print """stype must be either 'pole-dipole', 'dipole-dipole' or 'gradient'. """
return SrcList
# Add z coordinate nz = mesh.vectorNz endp = np.c_[np.asarray(temp), np.ones(2).T * nz[-1]] # Create dipole survey receivers and plot nrx = 10 ab = 40 a = 20 # Evenly distribute transmitters for now and put on surface dplen = np.sqrt(np.sum((endp[1, :] - endp[0, :])**2)) dp_x = (endp[1, 0] - endp[0, 0]) / dplen dp_y = (endp[1, 1] - endp[0, 1]) / dplen nstn = np.floor(dplen / ab) stn_x = endp[0, 0] + np.cumsum(np.ones(nstn) * dp_x * ab) stn_y = endp[0, 1] + np.cumsum(np.ones(nstn) * dp_y * ab) plt.scatter(stn_x, stn_y, s=100, c='w') M = np.c_[stn_x - a * dp_x, stn_y - a * dp_y, np.ones(nstn).T * nz[-1]] N = np.c_[stn_x + a * dp_x, stn_y + a * dp_y, np.ones(nstn).T * nz[-1]] plt.scatter(M[:, 0], M[:, 1], s=10, c='r') plt.scatter(N[:, 0], N[:, 1], s=10, c='b') #%% Create inversion parameter Rx = DC.RxDipole(M, N)
def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
from SimPEG import np
import re
"""
Load in endpoints and survey specifications to generate Tx, Rx location
stations.
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
Output:
:param Tx, Rx -> List objects for each tx location
Lines: P1x, P1y, P1z, P2x, P2y, P2z
Created on Wed December 9th, 2015
@author: dominiquef
"""
def xy_2_r(x1,x2,y1,y2):
r = np.sqrt( np.sum((x2 - x1)**2 + (y2 - y1)**2) )
return r
## Evenly distribute electrodes and put on surface
# Mesure survey length and direction
dl_len = xy_2_r(endl[0,0],endl[1,0],endl[0,1],endl[1,1])
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 )
# 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
# 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]]
## Build list of Tx-Rx locations depending on survey type
# Dipole-dipole: Moving tx with [a] spacing -> [AB a MN1 a MN2 ... a MNn]
# Pole-dipole: Moving pole on one end -> [A a MN1 a MN2 ... MNn a B]
Tx = []
Rx = []
if not re.match(stype,'gradient'):
for ii in range(0, int(nstn)-1):
if re.match(stype,'dpdp'):
tx = np.c_[M[ii,:],N[ii,:]]
elif re.match(stype,'pdp'):
tx = np.c_[M[ii,:],M[ii,:]]
#Rx.append(np.c_[M[ii+1:indx,:],N[ii+1:indx,:]])
# Current elctrode seperation
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])
# 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
# 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]]
Rx.append(np.c_[P1,P2])
Tx.append(tx)
#==============================================================================
# elif re.match(stype,'dpdp'):
#
# for ii in range(0, int(nstn)-2):
#
# indx = np.min([ii+n+1,nstn])
# Tx.append(np.c_[M[ii,:],N[ii,:]])
# Rx.append(np.c_[M[ii+2:indx,:],N[ii+2:indx,:]])
#==============================================================================
elif re.match(stype,'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
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
max_x = endl[1,0] - dl_x * b
max_y = endl[1,1] - dl_y * b
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 )
# 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
# Define number of cross lines
nlin = int(np.floor( box_w / a ))
lind = range(-nlin,nlin+1)
ngrad = nstn * len(lind)
rx = np.zeros([ngrad,6])
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
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]]
rx[(ii*nstn):((ii+1)*nstn),:] = np.c_[M,N]
Rx.append(rx)
else:
print """stype must be either 'pdp', 'dpdp' or 'gradient'. """
return Tx, Rx
def gen_DCIPsurvey(endl, mesh, stype, a, b, n):
"""
Load in endpoints and survey specifications to generate Tx, Rx location
stations.
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
Output:
:param Tx, Rx -> List objects for each tx location
Lines: P1x, P1y, P1z, P2x, P2y, P2z
Created on Wed December 9th, 2015
@author: dominiquef
!! Require clean up to deal with DCsurvey
"""
from SimPEG import np
def xy_2_r(x1,x2,y1,y2):
r = np.sqrt( np.sum((x2 - x1)**2 + (y2 - y1)**2) )
return r
## Evenly distribute electrodes and put on surface
# Mesure survey length and direction
dl_len = xy_2_r(endl[0,0],endl[1,0],endl[0,1],endl[1,1])
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 )
# 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
if mesh.dim==2:
ztop = mesh.vectorNy[-1]
# Create line of P1 locations
M = np.c_[stn_x, np.ones(nstn).T*ztop]
# Create line of P2 locations
N = np.c_[stn_x+a*dl_x, np.ones(nstn).T*ztop]
elif mesh.dim==3:
ztop = mesh.vectorNz[-1]
# Create line of P1 locations
M = np.c_[stn_x, stn_y, np.ones(nstn).T*ztop]
# Create line of P2 locations
N = np.c_[stn_x+a*dl_x, stn_y+a*dl_y, np.ones(nstn).T*ztop]
## Build list of Tx-Rx locations depending on survey type
# Dipole-dipole: Moving tx with [a] spacing -> [AB a MN1 a MN2 ... a MNn]
# Pole-dipole: Moving pole on one end -> [A a MN1 a MN2 ... MNn a B]
SrcList = []
if stype != 'gradient':
for ii in range(0, int(nstn)-1):
if stype == 'dipole-dipole':
tx = np.c_[M[ii,:],N[ii,:]]
elif stype == 'pole-dipole':
tx = np.c_[M[ii,:],M[ii,:]]
else:
raise Exception('The stype must be "dipole-dipole" or "pole-dipole"')
# Rx.append(np.c_[M[ii+1:indx,:],N[ii+1:indx,:]])
# Current elctrode seperation
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])
# 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
# Create receiver poles
if mesh.dim==3:
# Create line of P1 locations
P1 = np.c_[stn_x, stn_y, np.ones(nstn).T*ztop]
# Create line of P2 locations
P2 = np.c_[stn_x+a*dl_x, stn_y+a*dl_y, np.ones(nstn).T*ztop]
rxClass = DC.Rx.Dipole(P1, P2)
elif mesh.dim==2:
# Create line of P1 locations
P1 = np.c_[stn_x, np.ones(nstn).T*ztop]
# Create line of P2 locations
P2 = np.c_[stn_x+a*dl_x, np.ones(nstn).T*ztop]
rxClass = DC.Rx.Dipole_ky(P1, P2)
if stype == 'dipole-dipole':
srcClass = DC.Src.Dipole([rxClass], M[ii,:],N[ii,:])
elif stype == 'pole-dipole':
srcClass = DC.Src.Pole([rxClass], M[ii,:])
SrcList.append(srcClass)
elif stype == '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
# Get the edge limit of survey area
min_x = endl[0,0] + dl_x * b
min_y = endl[0,1] + dl_y * b
max_x = endl[1,0] - dl_x * b
max_y = endl[1,1] - dl_y * b
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 )
# 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
# Define number of cross lines
nlin = int(np.floor( box_w / a ))
lind = list(range(-nlin,nlin+1))
ngrad = nstn * len(lind)
rx = np.zeros([ngrad,6])
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
M = np.c_[ lxx, lyy , np.ones(nstn).T*ztop]
N = np.c_[ lxx+a*dl_x, lyy+a*dl_y, np.ones(nstn).T*ztop]
rx[(ii*nstn):((ii+1)*nstn),:] = np.c_[M,N]
if mesh.dim==3:
rxClass = DC.Rx.Dipole(rx[:,:3], rx[:,3:])
elif mesh.dim==2:
M = M[:,[0,2]]
N = N[:,[0,2]]
rxClass = DC.Rx.Dipole_ky(rx[:,[0,2]], rx[:,[3,5]])
srcClass = DC.Src.Dipole([rxClass], M[0,:], N[-1,:])
SrcList.append(srcClass)
else:
print("""stype must be either 'pole-dipole', 'dipole-dipole' or 'gradient'. """)
return SrcList
ymin = np.min(rxLoc[:, 1])
ymax = np.max(rxLoc[:, 1])
var = np.c_[np.r_[xmin, ymin], np.r_[xmax, ymin], np.r_[xmin, ymax]]
var = np.c_[var.T, np.ones(3) * mesh.vectorCCz[-1]]
# First put a tile on both corners of the mesh
indx = Utils.closestPoints(mesh, var)
endl = np.c_[mesh.gridCC[indx, 0], mesh.gridCC[indx, 1]]
dx = np.median(mesh.hx)
# Add intermediate tiles until the min_Olap is respected
# First in the x-direction
lx = np.floor((max_mcell / mesh.nCz)**0.5)
ntile = 2
Olap = -1
while Olap < min_Olap:
ntile += 1
# Set location of SW corners
#x0 = np.c_[xmin,xmax-lx*dx]
dx_t = np.round((endl[1, 0] - endl[0, 0]) / ((ntile - 1) * dx))
x1 = np.r_[endl[0, 0], endl[0, 0] + np.cumsum(
(np.ones(ntile - 2)) * dx_t * dx), endl[1, 0]]
x2 = x1 + lx * dx
def interpFFT(x, y, m):
"""
Load in a 2D grid and resample
OUTPUT:
m_out
"""
from SimPEG import np, sp
import scipy.signal as sn
# Add padding values by reflection (2**n)
lenx = np.round(np.log2(2 * len(x)))
npadx = int(np.floor((2**lenx - len(x)) / 2.))
#Create hemming taper
if np.mod(npadx * 2 + len(x), 2) != 0:
oddx = 1
else:
oddx = 0
tap0 = sn.hamming(npadx * 2)
tapl = sp.spdiags(tap0[0:npadx], 0, npadx, npadx)
tapr = sp.spdiags(tap0[npadx:], 0, npadx, npadx + oddx)
# Mirror the 2d data over the half lenght and apply 0-taper
mpad = np.hstack(
[np.fliplr(m[:, 0:npadx]) * tapl, m,
np.fliplr(m[:, -npadx:]) * tapr])
# Repeat along the second dimension
leny = np.round(np.log2(2 * len(y)))
npady = int(np.floor((2**leny - len(y)) / 2.))
#Create hemming taper
if np.mod(npady * 2 + len(y), 2) != 0:
oddy = 1
else:
oddy = 0
tap0 = sn.hamming(npady * 2)
tapu = sp.spdiags(tap0[0:npady], 0, npady, npady)
tapd = sp.spdiags(tap0[npady:], 0, npady + oddy, npady)
mpad = np.vstack([
tapu * np.flipud(mpad[0:npady, :]), mpad,
tapd * np.flipud(mpad[-npady:, :])
])
# Compute FFT
FFTm = np.fft.fft2(mpad)
# Do an FFT shift
FFTshift = np.fft.fftshift(FFTm)
# Pad high frequencies with zeros to increase the sampling rate
py = int(FFTm.shape[0] / 2)
px = int(FFTm.shape[1] / 2)
FFTshift = np.hstack([
np.zeros((FFTshift.shape[0], px)), FFTshift,
np.zeros((FFTshift.shape[0], px))
])
FFTshift = np.vstack([
np.zeros((py, FFTshift.shape[1])), FFTshift,
np.zeros((py, FFTshift.shape[1]))
])
# Inverse shift
FFTm = np.fft.ifftshift(FFTshift)
# Compute inverse FFT
IFFTm = np.fft.ifft2(FFTm) * FFTm.size / mpad.size
m_out = np.real(IFFTm)
# Extract core
#m_out = np.real(IFFTm[npady*2:-(npady*2+oddy+1),npadx*2:-(npadx*2+oddx+1)])
m_out = m_out[npady * 2:-(npady + oddy) * 2, npadx * 2:-(npadx + oddx) * 2]
if np.mod(m.shape[0], 2) != 0:
m_out = m_out[:-1, :]
if np.mod(m.shape[1], 2) != 0:
m_out = m_out[:, :-1]
return m_out
