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03dd9915b7
Add example for mag Add example for grav
258 lines
7.7 KiB
Python
258 lines
7.7 KiB
Python
#%%
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from SimPEG import *
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import simpegPF as PF
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import pylab as plt
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import os
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#home_dir = 'C:\Users\dominiquef.MIRAGEOSCIENCE\Documents\GIT\SimPEG\simpegpf\simpegPF\Dev'
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#home_dir = 'C:\\Users\\dominiquef.MIRAGEOSCIENCE\\ownCloud\\Research\\Modelling\\Synthetic\\Nut_Cracker\\Induced_MAG3C'
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home_dir = '.\\'
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#home_dir = '.\\'
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inpfile = 'PYMAG3D_inv.inp'
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dsep = '\\'
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os.chdir(home_dir)
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## New scripts to be added to basecode
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#from fwr_MAG_data import fwr_MAG_data
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#from read_MAGfwr_inp import read_MAGfwr_inp
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#%%
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# Read input file
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[mshfile, obsfile, topofile, mstart, mref, magfile, wgtfile, chi, alphas, bounds, lpnorms] = PF.Magnetics.read_MAGinv_inp(home_dir + dsep + inpfile)
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# Load mesh file
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mesh = Mesh.TensorMesh.readUBC(mshfile)
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#mesh = Utils.meshutils.readUBCTensorMesh(mshfile)
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# Load in observation file
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survey = PF.Magnetics.readUBCmagObs(obsfile)
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rxLoc = survey.srcField.rxList[0].locs
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d = survey.dobs
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wd = survey.std
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ndata = survey.srcField.rxList[0].locs.shape[0]
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beta_in = 1e+5
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# Load in topofile or create flat surface
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if topofile == 'null':
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# All active
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actv = np.asarray(range(mesh.nC))
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else:
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topo = np.genfromtxt(topofile,skip_header=1)
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# Find the active cells
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actv = PF.Magnetics.getActiveTopo(mesh,topo,'N')
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nC = len(actv)
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# Create active map to go from reduce set to full
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actvMap = Maps.ActiveCells(mesh, actv, -100)
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# Creat reduced identity map
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idenMap = Maps.IdentityMap(nP = nC)
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# Load starting model file
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if isinstance(mstart, float):
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mstart = np.ones(nC) * mstart
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else:
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mstart = Utils.meshutils.readUBCTensorModel(mstart,mesh)
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mstart = mstart[actv]
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# Load reference file
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if isinstance(mref, float):
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mref = np.ones(nC) * mref
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else:
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mref = Utils.meshutils.readUBCTensorModel(mref,mesh)
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mref = mref[actv]
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# Get magnetization vector for MOF
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if magfile=='DEFAULT':
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M_xyz = PF.Magnetics.dipazm_2_xyz(np.ones(nC) * survey.srcField.param[1], np.ones(nC) * survey.srcField.param[2])
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else:
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M_xyz = np.genfromtxt(magfile,delimiter=' \n',dtype=np.str,comments='!')
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# Get index of the center
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midx = int(mesh.nCx/2)
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midy = int(mesh.nCy/2)
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# Get distance weighting function
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#==============================================================================
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# wr = PF.Magnetics.get_dist_wgt(mesh,rxLoc,actv,3.,np.min(mesh.hx)/4)
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# #wrMap = PF.BaseMag.WeightMap(nC, wr)
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#==============================================================================
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#%% Plot obs data
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PF.Magnetics.plot_obs_2D(rxLoc,d,wd,'Observed Data')
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#%% Run inversion
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prob = PF.Magnetics.MagneticIntegral(mesh, mapping = idenMap, actInd = actv)
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prob.solverOpts['accuracyTol'] = 1e-4
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#survey = Survey.LinearSurvey()
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survey.pair(prob)
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#survey.makeSyntheticData(data, std=0.01)
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#survey.dobs=d
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#survey.mtrue = model
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# Write out the predicted
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pred = prob.fields(mstart)
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PF.Magnetics.writeUBCobs(home_dir + dsep + 'Pred.dat',survey,pred)
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wr = np.sum(prob.G**2.,axis=0)**0.5
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wr = ( wr/np.max(wr) )
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wr_out = actvMap * wr
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plt.figure()
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ax = plt.subplot()
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mesh.plotSlice(wr_out, ax = ax, normal = 'Y', ind=midx ,clim = (-1e-3, wr.max()))
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plt.title('Distance weighting')
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plt.xlabel('x');plt.ylabel('z')
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plt.gca().set_aspect('equal', adjustable='box')
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reg = Regularization.Simple(mesh, indActive = actv, mapping = idenMap)
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reg.mref = mref
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reg.wght = wr
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#reg.alpha_s = 1.
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# Create pre-conditioner
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diagA = np.sum(prob.G**2.,axis=0) + beta_in*(reg.W.T*reg.W).diagonal()*wr
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PC = Utils.sdiag(diagA**-1.)
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dmis = DataMisfit.l2_DataMisfit(survey)
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dmis.Wd = 1/wd
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opt = Optimization.ProjectedGNCG(maxIter=10,lower=0.,upper=1., maxIterCG= 20, tolCG = 1e-3)
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opt.approxHinv = PC
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# opt = Optimization.InexactGaussNewton(maxIter=6)
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invProb = InvProblem.BaseInvProblem(dmis, reg, opt, beta = beta_in)
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beta = Directives.BetaSchedule(coolingFactor=2, coolingRate=1)
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#betaest = Directives.BetaEstimate_ByEig()
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target = Directives.TargetMisfit()
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inv = Inversion.BaseInversion(invProb, directiveList=[beta,target])
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m0 = mstart
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# Run inversion
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mrec = inv.run(m0)
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m_out = actvMap*mrec
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# Write result
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Mesh.TensorMesh.writeModelUBC(mesh,'SimPEG_inv_l2l2.sus',m_out)
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#Utils.meshutils.writeUBCTensorModel(home_dir+dsep+'wr.dat',mesh,wr_out)
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# Plot predicted
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pred = prob.fields(mrec)
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#PF.Magnetics.plot_obs_2D(rxLoc,pred,wd,'Predicted Data')
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#PF.Magnetics.plot_obs_2D(rxLoc,(d-pred),wd,'Residual Data')
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print "Final misfit:" + str(np.sum( ((d-pred)/wd)**2. ) )
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#%% Plot out a section of the model
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yslice = midx
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plt.figure()
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ax = plt.subplot(221)
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mesh.plotSlice(m_out, ax = ax, normal = 'Z', ind=-5, clim = (-1e-3, mrec.max()))
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plt.plot(np.array([mesh.vectorCCx[0],mesh.vectorCCx[-1]]), np.array([mesh.vectorCCy[yslice],mesh.vectorCCy[yslice]]),c='w',linestyle = '--')
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plt.title('Z: ' + str(mesh.vectorCCz[-5]) + ' m')
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plt.xlabel('x');plt.ylabel('z')
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plt.gca().set_aspect('equal', adjustable='box')
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ax = plt.subplot(222)
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mesh.plotSlice(m_out, ax = ax, normal = 'Z', ind=-8, clim = (-1e-3, mrec.max()))
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plt.plot(np.array([mesh.vectorCCx[0],mesh.vectorCCx[-1]]), np.array([mesh.vectorCCy[yslice],mesh.vectorCCy[yslice]]),c='w',linestyle = '--')
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plt.title('Z: ' + str(mesh.vectorCCz[-8]) + ' m')
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plt.xlabel('x');plt.ylabel('z')
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plt.gca().set_aspect('equal', adjustable='box')
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ax = plt.subplot(212)
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mesh.plotSlice(m_out, ax = ax, normal = 'Y', ind=yslice, clim = (-1e-3, mrec.max()))
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plt.title('Cross Section')
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plt.xlabel('x');plt.ylabel('z')
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plt.gca().set_aspect('equal', adjustable='box')
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#%% Run one more round for sparsity
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phim = invProb.phi_m_last
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phid = invProb.phi_d
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reg = Regularization.Sparse(mesh, indActive = actv, mapping = idenMap)
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reg.recModel = mrec
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reg.mref = mref
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reg.wght = wr
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reg.eps = 1e-5
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reg.p = lpnorms[0]
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reg.qx = lpnorms[1]
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reg.qz = lpnorms[2]
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reg.qy = lpnorms[3]
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diagA = np.sum(prob.G**2.,axis=0) + beta_in*(reg.W.T*reg.W).diagonal()*(wr)
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PC = Utils.sdiag(diagA**-1.)
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#reg.alpha_s = 1.
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dmis = DataMisfit.l2_DataMisfit(survey)
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dmis.Wd = wd
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opt = Optimization.ProjectedGNCG(maxIter=10 ,lower=0.,upper=1., maxIterCG= 10, tolCG = 1e-4)
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opt.approxHinv = PC
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#opt.phim_last = reg.eval(mrec)
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# opt = Optimization.InexactGaussNewton(maxIter=6)
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invProb = InvProblem.BaseInvProblem(dmis, reg, opt, beta = invProb.beta)
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beta = Directives.BetaSchedule(coolingFactor=1, coolingRate=1)
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#betaest = Directives.BetaEstimate_ByEig()
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target = Directives.TargetMisfit()
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IRLS =Directives.update_IRLS( phi_m_last = phim, phi_d_last = phid )
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inv = Inversion.BaseInversion(invProb, directiveList=[beta,IRLS])
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m0 = mrec
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# Run inversion
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mrec = inv.run(m0)
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m_out = actvMap*mrec
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Mesh.TensorMesh.writeModelUBC(mesh,'SimPEG_inv_l0l2.sus',m_out)
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pred = prob.fields(mrec)
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#%% Plot obs data
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PF.Magnetics.plot_obs_2D(rxLoc,pred,wd,'Predicted Data')
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PF.Magnetics.plot_obs_2D(rxLoc,d,wd,'Observed Data')
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print "Final misfit:" + str(np.sum( ((d-pred)/wd)**2. ) )
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#%% Plot out a section of the model
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yslice = midx
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plt.figure()
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ax = plt.subplot(221)
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mesh.plotSlice(m_out, ax = ax, normal = 'Z', ind=-5, clim = (-1e-3, mrec.max()))
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plt.plot(np.array([mesh.vectorCCx[0],mesh.vectorCCx[-1]]), np.array([mesh.vectorCCy[yslice],mesh.vectorCCy[yslice]]),c='w',linestyle = '--')
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plt.title('Z: ' + str(mesh.vectorCCz[-5]) + ' m')
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plt.xlabel('x');plt.ylabel('z')
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plt.gca().set_aspect('equal', adjustable='box')
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ax = plt.subplot(222)
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mesh.plotSlice(m_out, ax = ax, normal = 'Z', ind=-8, clim = (-1e-3, mrec.max()))
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plt.plot(np.array([mesh.vectorCCx[0],mesh.vectorCCx[-1]]), np.array([mesh.vectorCCy[yslice],mesh.vectorCCy[yslice]]),c='w',linestyle = '--')
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plt.title('Z: ' + str(mesh.vectorCCz[-8]) + ' m')
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plt.xlabel('x');plt.ylabel('z')
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plt.gca().set_aspect('equal', adjustable='box')
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ax = plt.subplot(212)
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mesh.plotSlice(m_out, ax = ax, normal = 'Y', ind=yslice, clim = (-1e-3, mrec.max()))
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plt.title('Cross Section')
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plt.xlabel('x');plt.ylabel('z')
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plt.gca().set_aspect('equal', adjustable='box') |