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seismic_CPML_3D_viscoelastic_MPI.f90
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seismic_CPML_3D_viscoelastic_MPI.f90
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!
! SEISMIC_CPML Version 1.2, April 2015.
!
! Copyright CNRS, France.
! Contributors: Roland Martin, roland DOT martin aT get DOT obs-mip DOT fr
! and Dimitri Komatitsch, komatitsch aT lma DOT cnrs-mrs DOT fr
!
! April 2015: Dimitri Komatitsch added support for the SolvOpt algorithm to compute
! the attenuation parameters in an optimized way. If you use it please cite:
!
! @Article{BlKoChLoXi15,
! Title = {Positivity-preserving highly-accurate optimization of the {Z}ener viscoelastic model, with application
! to wave propagation in the presence of strong attenuation},
! Author = {\'Emilie Blanc and Dimitri Komatitsch and Emmanuel Chaljub and Bruno Lombard and Zhinan Xie},
! Journal = {Geophysical Journal International},
! Year = {2015},
! Note = {in press.}}
!
! This software is a computer program whose purpose is to solve
! the three-dimensional isotropic viscoelastic wave equation
! using a fourth order finite-difference method with Convolutional Perfectly Matched Layer (C-PML) conditions.
!
! This program is free software; you can redistribute it and/or modify
! it under the terms of the GNU General Public License as published by
! the Free Software Foundation; either version 3 of the License, or
! (at your option) any later version.
!
! This program is distributed in the hope that it will be useful,
! but WITHOUT ANY WARRANTY; without even the implied warranty of
! MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the
! GNU General Public License for more details.
!
! You should have received a copy of the GNU General Public License along
! with this program; if not, write to the Free Software Foundation, Inc.,
! 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301 USA.
!
! The full text of the license is available in file "LICENSE".
program seismic_visco_CPML_3D_MPI_OpenMP
! 3D fourth order viscoelastic finite-difference code in velocity and stress formulation
! with Convolutional-PML (C-PML) absorbing conditions using 2 mechanisms of attenuation
! with 6 equations per mechanism.
! Roland Martin, University of Pau, France, October 2009.
! based on the elastic code of Komatitsch and Martin, 2007.
! April 2015: Dimitri Komatitsch added support for the SolvOpt algorithm to compute
! the attenuation parameters in an optimized way.
! The fourth-order staggered-grid formulation of Madariaga (1976) and Virieux (1986) is used.
! *BEWARE* that the attenuation model implemented below is that of J. M. Carcione,
! Seismic modeling in viscoelastic media, Geophysics, vol. 58(1), p. 110-120 (1993), which is NON causal,
! i.e., waves speed up instead of slowing down when turning attenuation on.
! This comes from the fact that in that model the relaxed state at zero frequency is used as a reference instead of
! the unrelaxed state at infinite frequency. These days a causal model should be used instead,
! i.e. one using the unrelaxed state at infinite frequency as a reference.
! The C-PML implementation is based in part on formulas given in Roden and Gedney (2000).
!
! Parallel implementation based on MPI.
! The C-PML implementation is based in part on formulas given in Roden and Gedney (2000).
! If you use this code for your own research, please cite some (or all) of these articles:
!
! @Article{BlKoChLoXi15,
! Title = {Positivity-preserving highly-accurate optimization of the {Z}ener viscoelastic model, with application
! to wave propagation in the presence of strong attenuation},
! Author = {\'Emilie Blanc and Dimitri Komatitsch and Emmanuel Chaljub and Bruno Lombard and Zhinan Xie},
! Journal = {Geophysical Journal International},
! Year = {2015},
! Note = {in press.}}
!
! @ARTICLE{MaKo09,
! author = {Roland Martin and Dimitri Komatitsch},
! title = {An unsplit convolutional perfectly matched layer technique improved
! at grazing incidence for the viscoelastic wave equation},
! journal = {Geophysical Journal International},
! year = {2009},
! volume = {179},
! pages = {333-344},
! number = {1},
! doi = {10.1111/j.1365-246X.2009.04278.x}}
!
! @ARTICLE{MaKoEz08,
! author = {Roland Martin and Dimitri Komatitsch and Abdela\^aziz Ezziani},
! title = {An unsplit convolutional perfectly matched layer improved at grazing
! incidence for seismic wave equation in poroelastic media},
! journal = {Geophysics},
! year = {2008},
! volume = {73},
! pages = {T51-T61},
! number = {4},
! doi = {10.1190/1.2939484}}
!
! @ARTICLE{MaKoGe08,
! author = {Roland Martin and Dimitri Komatitsch and Stephen D. Gedney},
! title = {A variational formulation of a stabilized unsplit convolutional perfectly
! matched layer for the isotropic or anisotropic seismic wave equation},
! journal = {Computer Modeling in Engineering and Sciences},
! year = {2008},
! volume = {37},
! pages = {274-304},
! number = {3}}
!
! @ARTICLE{KoMa07,
! author = {Dimitri Komatitsch and Roland Martin},
! title = {An unsplit convolutional {P}erfectly {M}atched {L}ayer improved
! at grazing incidence for the seismic wave equation},
! journal = {Geophysics},
! year = {2007},
! volume = {72},
! number = {5},
! pages = {SM155-SM167},
! doi = {10.1190/1.2757586}}
!
! The original CPML technique for Maxwell's equations is described in:
!
! @ARTICLE{RoGe00,
! author = {J. A. Roden and S. D. Gedney},
! title = {Convolution {PML} ({CPML}): {A}n Efficient {FDTD} Implementation
! of the {CFS}-{PML} for Arbitrary Media},
! journal = {Microwave and Optical Technology Letters},
! year = {2000},
! volume = {27},
! number = {5},
! pages = {334-339},
! doi = {10.1002/1098-2760(20001205)27:5 < 334::AID-MOP14>3.0.CO;2-A}}
!
! To display the results as color images in the selected 2D cut plane, use:
!
! " display image*.gif " or " gimp image*.gif "
!
! or
!
! " montage -geometry +0+3 -rotate 90 -tile 1x21 image*Vx*.gif allfiles_Vx.gif "
! " montage -geometry +0+3 -rotate 90 -tile 1x21 image*Vy*.gif allfiles_Vy.gif "
! then " display allfiles_Vx.gif " or " gimp allfiles_Vx.gif "
! then " display allfiles_Vy.gif " or " gimp allfiles_Vy.gif "
!
! IMPORTANT : all our CPML codes work fine in single precision as well (which is significantly faster).
! If you want you can thus force automatic conversion to single precision at compile time
! or change all the declarations and constants in the code from double precision to single.
use mpi
implicit none
! total number of grid points in each direction of the grid
integer, parameter :: NX = 210
integer, parameter :: NY = 800
integer, parameter :: NZ = 220 ! even number in order to cut along Z axis
! number of processes used in the MPI run
! and local number of points (for simplicity we cut the mesh along Z only)
integer, parameter :: NPROC = 4 !! 20
integer, parameter :: NZ_LOCAL = NZ / NPROC
! size of a grid cell
double precision, parameter :: DELTAX = 4.d0, ONE_OVER_DELTAX = 1.d0 / DELTAX
double precision, parameter :: DELTAY = DELTAX, DELTAZ = DELTAX
double precision, parameter :: ONE_OVER_DELTAY = ONE_OVER_DELTAX, ONE_OVER_DELTAZ = ONE_OVER_DELTAX
double precision, parameter :: ONE=1.d0,TWO=2.d0, DIM=3.d0
! P-velocity, S-velocity and density
double precision, parameter :: cp = 3000.d0
double precision, parameter :: cs = 2000.d0
double precision, parameter :: rho = 2000.d0
double precision, parameter :: mu = rho*cs*cs
double precision, parameter :: lambda = rho*(cp*cp - 2.d0*cs*cs)
double precision, parameter :: lambdaplustwomu = rho*cp*cp
! total number of time steps
integer, parameter :: NSTEP = 100000
! time step in seconds
double precision, parameter :: DELTAT = 4.d-4
! parameters for the source
double precision, parameter :: f0 = 18.d0
double precision, parameter :: t0 = 1.20d0 / f0
double precision, parameter :: factor = 1.d7
! parameters for attenuation
! number of standard linear solids
integer, parameter :: N_SLS = 2
! Qp approximately equal to 13, Qkappa approximately to 20 and Qmu / Qs approximately to 10
double precision, parameter :: QKappa_att = 20.d0, QMu_att = 10.d0
double precision, parameter :: f0_attenuation = 16 ! in Hz
! flags to add PML layers to the edges of the grid
logical, parameter :: USE_PML_XMIN = .true.
logical, parameter :: USE_PML_XMAX = .true.
logical, parameter :: USE_PML_YMIN = .true.
logical, parameter :: USE_PML_YMAX = .true.
logical, parameter :: USE_PML_ZMIN = .true.
logical, parameter :: USE_PML_ZMAX = .true.
! thickness of the PML layer in grid points
integer, parameter :: NPOINTS_PML = 10
! source
! integer, parameter :: ISOURCE = NX - 2*NPOINTS_PML - 1
integer, parameter :: ISOURCE = NPOINTS_PML+20
integer, parameter :: JSOURCE = NY / 5 + 1
double precision, parameter :: xsource = (ISOURCE) * DELTAX
double precision, parameter :: ysource = (JSOURCE) * DELTAY
! angle of source force clockwise with respect to vertical (Y) axis
double precision, parameter :: ANGLE_FORCE = 0.d0
! receivers
integer, parameter :: NREC = 3
double precision, parameter :: xdeb = xsource - 100.d0 ! first receiver x in meters
double precision, parameter :: ydeb = 2300.d0 ! first receiver y in meters
double precision, parameter :: xfin = xsource ! last receiver x in meters
double precision, parameter :: yfin = 300.d0 ! last receiver y in meters
! display information on the screen from time to time
integer, parameter :: IT_DISPLAY = 10000
! value of PI
double precision, parameter :: PI = 3.141592653589793238462643d0
! conversion from degrees to radians
double precision, parameter :: DEGREES_TO_RADIANS = PI / 180.d0
! zero
double precision, parameter :: ZERO = 0.d0
! large value for maximum
double precision, parameter :: HUGEVAL = 1.d+30
! velocity threshold above which we consider that the code became unstable
double precision, parameter :: STABILITY_THRESHOLD = 1.d+25
! power to compute d0 profile
double precision, parameter :: NPOWER = 2.d0
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-11
double precision, parameter :: K_MAX_PML = 7.d0
double precision, parameter :: ALPHA_MAX_PML = 2.d0*PI*(f0/2.d0) ! from Festa and Vilotte
! arrays for the memory variables
! could declare these arrays in PML only to save a lot of memory, but proof of concept only here
double precision, dimension(0:NX+1,0:NY+1,-1:NZ_LOCAL+2) :: &
memory_dvx_dx, &
memory_dvx_dy, &
memory_dvx_dz, &
memory_dvy_dx, &
memory_dvy_dy, &
memory_dvy_dz, &
memory_dvz_dx, &
memory_dvz_dy, &
memory_dvz_dz, &
memory_dsigmaxx_dx, &
memory_dsigmayy_dy, &
memory_dsigmazz_dz, &
memory_dsigmaxy_dx, &
memory_dsigmaxy_dy, &
memory_dsigmaxz_dx, &
memory_dsigmaxz_dz, &
memory_dsigmayz_dy, &
memory_dsigmayz_dz
double precision :: &
value_dvx_dx, &
value_dvx_dy, &
value_dvx_dz, &
value_dvy_dx, &
value_dvy_dy, &
value_dvy_dz, &
value_dvz_dx, &
value_dvz_dy, &
value_dvz_dz, &
value_dsigmaxx_dx, &
value_dsigmayy_dy, &
value_dsigmazz_dz, &
value_dsigmaxy_dx, &
value_dsigmaxy_dy, &
value_dsigmaxz_dx, &
value_dsigmaxz_dz, &
value_dsigmayz_dy, &
value_dsigmayz_dz
double precision :: duxdx,duxdy,duxdz,duydx,duydy,duydz,duzdx,duzdy,duzdz,div
! 1D arrays for the damping profiles
double precision, dimension(1:NX) :: d_x,K_x,alpha_x,a_x,b_x,d_x_half,K_x_half,alpha_x_half,a_x_half,b_x_half
double precision, dimension(1:NY) :: d_y,K_y,alpha_y,a_y,b_y,d_y_half,K_y_half,alpha_y_half,a_y_half,b_y_half
double precision, dimension(1:NZ) :: d_z,K_z,alpha_z,a_z,b_z,d_z_half,K_z_half,alpha_z_half,a_z_half,b_z_half
! PML
double precision thickness_PML_x,thickness_PML_y,thickness_PML_z
double precision xoriginleft,xoriginright,yoriginbottom,yorigintop,zoriginbottom,zorigintop
double precision Rcoef,d0_x,d0_y,d0_z,xval,yval,zval,abscissa_in_PML,abscissa_normalized
! change dimension of Z axis to add two planes for MPI
double precision, dimension(0:NX+1,0:NY+1,-1:NZ_LOCAL+2) :: vx,vy,vz,sigmaxx,sigmayy,sigmazz,sigmaxy,sigmaxz,sigmayz
double precision, dimension(0:NX+1,0:NY+1,-1:NZ_LOCAL+2) :: sigmaxx_R,sigmayy_R,sigmazz_R,sigmaxy_R,sigmaxz_R,sigmayz_R
double precision, dimension(N_SLS,0:NX+1,0:NY+1,-1:NZ_LOCAL+2) :: e1,e11,e22,e12,e13,e23
integer, parameter :: number_of_arrays = 9 + 2*9 + 12
! for the source
double precision a,t,force_x,force_y,source_term
! for attenuation
double precision :: f_min_attenuation, f_max_attenuation
double precision, dimension(N_SLS) :: tau_epsilon_nu1,tau_sigma_nu1,tau_epsilon_nu2,tau_sigma_nu2
! for receivers
double precision distval,dist
integer, dimension(NREC) :: ix_rec,iy_rec
double precision, dimension(NREC) :: xrec,yrec
! for seismograms
double precision, dimension(NSTEP,NREC) :: sisvx,sisvy
! max amplitude for color snapshots
double precision max_amplitudeVx
double precision max_amplitudeVy
! for evolution of total energy in the medium
double precision :: epsilon_xx,epsilon_yy,epsilon_zz,epsilon_xy,epsilon_xz,epsilon_yz
double precision, dimension(NSTEP) :: total_energy,total_energy_kinetic,total_energy_potential
double precision :: local_energy_kinetic,local_energy_potential
integer :: irec
! precompute some parameters once and for all
double precision, parameter :: DELTAT_lambda = DELTAT*lambda
double precision, parameter :: DELTAT_mu = DELTAT*mu
double precision, parameter :: DELTAT_lambdaplus2mu = DELTAT*lambdaplustwomu
double precision, parameter :: DELTAT_over_rho = DELTAT/rho
double precision :: mul_relaxed,lambdal_relaxed,lambdalplus2mul_relaxed
double precision :: mul_unrelaxed,lambdal_unrelaxed,lambdalplus2mul_unrelaxed
double precision :: Un,Sn,Unp1,Mu_nu1,Mu_nu2
double precision :: phi_nu1(N_SLS)
double precision :: phi_nu2(N_SLS)
double precision :: tauinv,inv_tau_sigma_nu1(N_SLS)
double precision :: taumin,taumax,tau1,tau2,tau3,tau4
double precision :: inv_tau_sigma_nu2(N_SLS)
double precision :: tauinvUn
integer :: i,j,k,it,it2
double precision :: Vsolidnorm,Courant_number
! timer to count elapsed time
character(len=8) datein
character(len=10) timein
character(len=5) :: zone
integer, dimension(8) :: time_values
integer ihours,iminutes,iseconds,int_tCPU
double precision :: time_start,time_end,tCPU
! names of the time stamp files
character(len=150) outputname
! main I/O file
integer, parameter :: IOUT = 41
! array needed for MPI_RECV
integer, dimension(MPI_STATUS_SIZE) :: message_status
! tag of the message to send
integer, parameter :: message_tag = 0
! number of values to send or receive
integer, parameter :: number_of_values = 2*(NX+2)*(NY+2)
integer :: nb_procs,rank,code,rank_cut_plane,kmin,kmax,kglobal,offset_k,k2begin,kminus1end
integer :: sender_right_shift,receiver_right_shift,sender_left_shift,receiver_left_shift
!---
!--- program starts here
!---
! start MPI processes
call MPI_INIT(code)
! get total number of MPI processes in variable nb_procs
call MPI_COMM_SIZE(MPI_COMM_WORLD, nb_procs, code)
! get the rank of our process from 0 (master) to nb_procs-1 (workers)
call MPI_COMM_RANK(MPI_COMM_WORLD, rank, code)
! attenuation constants for standard linear solids
! nu1 is the dilatation/incompressibility mode (QKappa)
! nu2 is the shear mode (Qmu)
! array index (1) is the first standard linear solid, (2) is the second etc.
! from J. M. Carcione, Seismic modeling in viscoelastic media, Geophysics,
! vol. 58(1), p. 110-120 (1993) for two memory-variable mechanisms (page 112).
! Beware: these values implement specific values of the quality factors:
! Qp approximately equal to 13, Qkappa approximately to 20 and Qmu / Qs approximately to 10,
! which means very high attenuation, see that paper for details.
! tau_epsilon_nu1(1) = 0.0334d0
! tau_sigma_nu1(1) = 0.0303d0
! tau_epsilon_nu2(1) = 0.0352d0
! tau_sigma_nu2(1) = 0.0287d0
! tau_epsilon_nu1(2) = 0.0028d0
! tau_sigma_nu1(2) = 0.0025d0
! tau_epsilon_nu2(2) = 0.0029d0
! tau_sigma_nu2(2) = 0.0024d0
! from J. M. Carcione, D. Kosloff and R. Kosloff, Wave propagation simulation
! in a linear viscoelastic medium, Geophysical Journal International,
! vol. 95, p. 597-611 (1988) for two memory-variable mechanisms (page 604).
! Beware: these values implement specific values of the quality factors:
! Qkappa approximately to 27 and Qmu / Qs approximately to 20,
! which means very high attenuation, see that paper for details.
! tau_epsilon_nu1(1) = 0.0325305d0
! tau_sigma_nu1(1) = 0.0311465d0
! tau_epsilon_nu2(1) = 0.0332577d0
! tau_sigma_nu2(1) = 0.0304655d0
! tau_epsilon_nu1(2) = 0.0032530d0
! tau_sigma_nu1(2) = 0.0031146d0
! tau_epsilon_nu2(2) = 0.0033257d0
! tau_sigma_nu2(2) = 0.0030465d0
! f_min and f_max are computed as : f_max/f_min=12 and (log(f_min)+log(f_max))/2 = log(f0)
f_min_attenuation = exp(log(f0_attenuation)-log(12.d0)/2.d0)
f_max_attenuation = 12.d0 * f_min_attenuation
! use new SolvOpt nonlinear optimization with constraints from Emilie Blanc, Bruno Lombard and Dimitri Komatitsch
! to compute attenuation mechanisms
call compute_attenuation_coeffs(N_SLS,QKappa_att,f0_attenuation,f_min_attenuation,f_max_attenuation, &
tau_epsilon_nu1,tau_sigma_nu1)
call compute_attenuation_coeffs(N_SLS,QMu_att,f0_attenuation,f_min_attenuation,f_max_attenuation, &
tau_epsilon_nu2,tau_sigma_nu2)
if (rank == 0) then
print *
print *,'with new SolvOpt routine for attenuation:'
print *
print *,'N_SLS, QKappa_att, QMu_att = ',N_SLS, QKappa_att, QMu_att
print *,'f0_attenuation,f_min_attenuation,f_max_attenuation = ',f0_attenuation,f_min_attenuation,f_max_attenuation
print *,'tau_epsilon_nu1 = ',tau_epsilon_nu1
print *,'tau_sigma_nu1 = ',tau_sigma_nu1
print *,'tau_epsilon_nu2 = ',tau_epsilon_nu2
print *,'tau_sigma_nu2 = ',tau_sigma_nu2
print *
endif
tau1 = tau_sigma_nu1(1)/tau_epsilon_nu1(1)
tau2 = tau_sigma_nu2(1)/tau_epsilon_nu2(1)
tau3 = tau_sigma_nu1(2)/tau_epsilon_nu1(2)
tau4 = tau_sigma_nu2(2)/tau_epsilon_nu2(2)
taumax = max(1.d0/tau1,1.d0/tau2,1.d0/tau3,1.d0/tau4)
taumin = min(1.d0/tau1,1.d0/tau2,1.d0/tau3,1.d0/tau4)
inv_tau_sigma_nu1(1) = ONE / tau_sigma_nu1(1)
inv_tau_sigma_nu2(1) = ONE / tau_sigma_nu2(1)
inv_tau_sigma_nu1(2) = ONE / tau_sigma_nu1(2)
inv_tau_sigma_nu2(2) = ONE / tau_sigma_nu2(2)
phi_nu1(1) = (ONE - tau_epsilon_nu1(1)/tau_sigma_nu1(1)) / tau_sigma_nu1(1)
phi_nu2(1) = (ONE - tau_epsilon_nu2(1)/tau_sigma_nu2(1)) / tau_sigma_nu2(1)
phi_nu1(2) = (ONE - tau_epsilon_nu1(2)/tau_sigma_nu1(2)) / tau_sigma_nu1(2)
phi_nu2(2) = (ONE - tau_epsilon_nu2(2)/tau_sigma_nu2(2)) / tau_sigma_nu2(2)
Mu_nu1 = ONE - (ONE - tau_epsilon_nu1(1)/tau_sigma_nu1(1)) - (ONE - tau_epsilon_nu1(2)/tau_sigma_nu1(2))
Mu_nu2 = ONE - (ONE - tau_epsilon_nu2(1)/tau_sigma_nu2(1)) - (ONE - tau_epsilon_nu2(2)/tau_sigma_nu2(2))
! slice number for the cut plane in the middle of the mesh
rank_cut_plane = nb_procs/2 - 1
if (rank == rank_cut_plane) then
print *
print *,'3D elastic finite-difference code in velocity and stress formulation with C-PML'
print *
! display size of the model
print *
print *,'NX = ',NX
print *,'NY = ',NY
print *,'NZ = ',NZ
print *
print *,'NZ_LOCAL = ',NZ_LOCAL
print *,'NPROC = ',NPROC
print *
print *,'size of the model along X = ',(NX+1) * DELTAX
print *,'size of the model along Y = ',(NY+1) * DELTAY
print *,'size of the model along Y = ',(NZ+1) * DELTAZ
print *
print *,'Total number of grid points = ',(NX+2) * (NY+2) * (NZ+2)
print *,'Number of points of all the arrays = ',dble(NX+2)*dble(NY+2)*dble(NZ+2)*number_of_arrays
print *,'Size in GB of all the arrays = ',dble(NX+2)*dble(NY+2)*dble(NZ+2)*number_of_arrays*8.d0/(1024.d0*1024.d0*1024.d0)
print *
print *,'In each slice:'
print *
print *,'Total number of grid points = ',(NX+2) * (NY+2) * NZ_LOCAL
print *,'Number of points of the arrays = ',dble(NX+2)*dble(NY+2)*dble(NZ_LOCAL)*number_of_arrays
print *,'Size in GB of the arrays = ',dble(NX+2)*dble(NY+2)*dble(NZ_LOCAL)*number_of_arrays*8.d0/(1024.d0*1024.d0*1024.d0)
print *
endif
! check that code was compiled with the right number of slices
if (nb_procs /= NPROC) then
print *,'error in MPI number of slices: nb_procs,NPROC = ',nb_procs,NPROC,' but they should be equal'
stop 'nb_procs must be equal to NPROC'
endif
! we restrict ourselves to an even number of slices
! in order to have a cut plane in the middle of the mesh for visualization purposes
if (mod(nb_procs,2) /= 0) stop 'nb_procs must be even'
! check that we can cut along Z in an exact number of slices
if (mod(NZ,nb_procs) /= 0) stop 'NZ must be a multiple of nb_procs'
! check that a slice is at least as thick as a PML layer
if (NZ_LOCAL < NPOINTS_PML) stop 'NZ_LOCAL must be greater than NPOINTS_PML'
! offset of this slice when we cut along Z
offset_k = rank * NZ_LOCAL
!--- define profile of absorption in PML region
! thickness of the PML layer in meters
thickness_PML_x = NPOINTS_PML * DELTAX
thickness_PML_y = NPOINTS_PML * DELTAY
thickness_PML_z = NPOINTS_PML * DELTAZ
! reflection coefficient (INRIA report section 6.1) http://hal.inria.fr/docs/00/07/32/19/PDF/RR-3471.pdf
Rcoef = 0.0001d0
! check that NPOWER is okay
if (NPOWER < 1) stop 'NPOWER must be greater than 1'
! compute d0 from INRIA report section 6.1 http://hal.inria.fr/docs/00/07/32/19/PDF/RR-3471.pdf
d0_x = - (NPOWER + 1) * cp *dsqrt(taumax)* log(Rcoef) / (2.d0 * thickness_PML_x)
d0_y = - (NPOWER + 1) * cp *dsqrt(taumax)* log(Rcoef) / (2.d0 * thickness_PML_y)
d0_z = - (NPOWER + 1) * cp *dsqrt(taumax)* log(Rcoef) / (2.d0 * thickness_PML_z)
if (rank == rank_cut_plane) then
print *
print *,'d0_x = ',d0_x
print *,'d0_y = ',d0_y
print *,'d0_z = ',d0_z
endif
! PML
d_x(:) = ZERO
d_x_half(:) = ZERO
K_x(:) = 1.d0
K_x_half(:) = 1.d0
alpha_x(:) = ZERO
alpha_x_half(:) = ZERO
a_x(:) = ZERO
a_x_half(:) = ZERO
d_y(:) = ZERO
d_y_half(:) = ZERO
K_y(:) = 1.d0
K_y_half(:) = 1.d0
alpha_y(:) = ZERO
alpha_y_half(:) = ZERO
a_y(:) = ZERO
a_y_half(:) = ZERO
d_z(:) = ZERO
d_z_half(:) = ZERO
K_z(:) = 1.d0
K_z_half(:) = 1.d0
alpha_z(:) = ZERO
alpha_z_half(:) = ZERO
a_z(:) = ZERO
a_z_half(:) = ZERO
! damping in the X direction
! origin of the PML layer (position of right edge minus thickness, in meters)
xoriginleft = thickness_PML_x
xoriginright = (NX-1)*DELTAX - thickness_PML_x
do i = 1,NX
! abscissa of current grid point along the damping profile
xval = DELTAX * dble(i-1)
!---------- xmin edge
if (USE_PML_XMIN) then
! define damping profile at the grid points
abscissa_in_PML = xoriginleft - xval
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_x
d_x(i) = d0_x * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_x(i) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_x(i) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
! define damping profile at half the grid points
abscissa_in_PML = xoriginleft - (xval + DELTAX/2.d0)
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_x
d_x_half(i) = d0_x * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_x_half(i) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_x_half(i) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
endif
!---------- xmax edge
if (USE_PML_XMAX) then
! define damping profile at the grid points
abscissa_in_PML = xval - xoriginright
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_x
d_x(i) = d0_x * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_x(i) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_x(i) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
! define damping profile at half the grid points
abscissa_in_PML = xval + DELTAX/2.d0 - xoriginright
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_x
d_x_half(i) = d0_x * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_x_half(i) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_x_half(i) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
endif
! just in case, for -5 at the end
if (alpha_x(i) < ZERO) alpha_x(i) = ZERO
if (alpha_x_half(i) < ZERO) alpha_x_half(i) = ZERO
b_x(i) = exp(- (d_x(i) / K_x(i) + alpha_x(i)) * DELTAT)
b_x_half(i) = exp(- (d_x_half(i) / K_x_half(i) + alpha_x_half(i)) * DELTAT)
! this to avoid division by zero outside the PML
if (abs(d_x(i)) > 1.d-6) a_x(i) = d_x(i) * (b_x(i) - 1.d0) / (K_x(i) * (d_x(i) + K_x(i) * alpha_x(i)))
if (abs(d_x_half(i)) > 1.d-6) a_x_half(i) = d_x_half(i) * &
(b_x_half(i) - 1.d0) / (K_x_half(i) * (d_x_half(i) + K_x_half(i) * alpha_x_half(i)))
enddo
! damping in the Y direction
! origin of the PML layer (position of right edge minus thickness, in meters)
yoriginbottom = thickness_PML_y
yorigintop = (NY-1)*DELTAY - thickness_PML_y
do j = 1,NY
! abscissa of current grid point along the damping profile
yval = DELTAY * dble(j-1)
!---------- ymin edge
if (USE_PML_YMIN) then
! define damping profile at the grid points
abscissa_in_PML = yoriginbottom - yval
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_y
d_y(j) = d0_y * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_y(j) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_y(j) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
! define damping profile at half the grid points
abscissa_in_PML = yoriginbottom - (yval + DELTAY/2.d0)
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_y
d_y_half(j) = d0_y * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_y_half(j) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_y_half(j) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
endif
!---------- ymax edge
if (USE_PML_YMAX) then
! define damping profile at the grid points
abscissa_in_PML = yval - yorigintop
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_y
d_y(j) = d0_y * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_y(j) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_y(j) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
! define damping profile at half the grid points
abscissa_in_PML = yval + DELTAY/2.d0 - yorigintop
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_y
d_y_half(j) = d0_y * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_y_half(j) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_y_half(j) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
endif
b_y(j) = exp(- (d_y(j) / K_y(j) + alpha_y(j)) * DELTAT)
b_y_half(j) = exp(- (d_y_half(j) / K_y_half(j) + alpha_y_half(j)) * DELTAT)
! this to avoid division by zero outside the PML
if (abs(d_y(j)) > 1.d-6) a_y(j) = d_y(j) * (b_y(j) - 1.d0) / (K_y(j) * (d_y(j) + K_y(j) * alpha_y(j)))
if (abs(d_y_half(j)) > 1.d-6) a_y_half(j) = d_y_half(j) * &
(b_y_half(j) - 1.d0) / (K_y_half(j) * (d_y_half(j) + K_y_half(j) * alpha_y_half(j)))
enddo
! damping in the Z direction
! origin of the PML layer (position of right edge minus thickness, in meters)
zoriginbottom = thickness_PML_z
zorigintop = (NZ-1)*DELTAZ - thickness_PML_z
do k = 1,NZ
! abscissa of current grid point along the damping profile
zval = DELTAZ * dble(k-1)
!---------- zmin edge
if (USE_PML_ZMIN) then
! define damping profile at the grid points
abscissa_in_PML = zoriginbottom - zval
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_z
d_z(k) = d0_z * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_z(k) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_z(k) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
! define damping profile at half the grid points
abscissa_in_PML = zoriginbottom - (zval + DELTAZ/2.d0)
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_z
d_z_half(k) = d0_z * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_z_half(k) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_z_half(k) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
endif
!---------- zmax edge
if (USE_PML_ZMAX) then
! define damping profile at the grid points
abscissa_in_PML = zval - zorigintop
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_z
d_z(k) = d0_z * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_z(k) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_z(k) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
! define damping profile at half the grid points
abscissa_in_PML = zval + DELTAZ/2.d0 - zorigintop
if (abscissa_in_PML >= ZERO) then
abscissa_normalized = abscissa_in_PML / thickness_PML_z
d_z_half(k) = d0_z * abscissa_normalized**NPOWER
! from Stephen Gedney's unpublished class notes for class EE699, lecture 8, slide 8-2
K_z_half(k) = 1.d0 + (K_MAX_PML - 1.d0) * abscissa_normalized**NPOWER
alpha_z_half(k) = ALPHA_MAX_PML * (1.d0 - abscissa_normalized)
endif
endif
b_z(k) = exp(- (d_z(k) / K_z(k) + alpha_z(k)) * DELTAT)
b_z_half(k) = exp(- (d_z_half(k) / K_z_half(k) + alpha_z_half(k)) * DELTAT)
! this to avoid division by zero outside the PML
if (abs(d_z(k)) > 1.d-6) a_z(k) = d_z(k) * (b_z(k) - 1.d0) / (K_z(k) * (d_z(k) + K_z(k) * alpha_z(k)))
if (abs(d_z_half(k)) > 1.d-6) a_z_half(k) = d_z_half(k) * &
(b_z_half(k) - 1.d0) / (K_z_half(k) * (d_z_half(k) + K_z_half(k) * alpha_z_half(k)))
enddo
if (rank == rank_cut_plane) then
! print position of the source
print *
print *,'Position of the source:'
print *
print *,'x = ',xsource
print *,'y = ',ysource
print *
! define location of receivers
print *
print *,'There are ',nrec,' receivers'
print *
! xspacerec = (xfin-xdeb) / dble(NREC-1)
! yspacerec = (yfin-ydeb) / dble(NREC-1)
! do irec=1,nrec
! xrec(irec) = xdeb + dble(irec-1)*xspacerec
! yrec(irec) = ydeb + dble(irec-1)*yspacerec
! enddo
xrec(1)=xsource+500.d0 ! first receiver x in meters
yrec(1)=ysource+500.d0 ! first receiver y in meters
xrec(2)=xsource ! first receiver x in meters
yrec(2)=ysource+2260.d0 ! first receiver y in meters
xrec(3)=xsource+500.d0 ! first receiver x in meters
yrec(3)=ysource+2260.d0 ! first receiver y in meters
! find closest grid point for each receiver
do irec=1,nrec
dist = HUGEVAL
do j = 1,NY
do i = 1,NX
distval = sqrt((DELTAX*dble(i) - xrec(irec))**2 + (DELTAY*dble(j) - yrec(irec))**2)
if (distval < dist) then
dist = distval
ix_rec(irec) = i
iy_rec(irec) = j
endif
enddo
enddo
print *,'receiver ',irec,' x_target,y_target = ',xrec(irec),yrec(irec)
print *,'closest grid point found at distance ',dist,' in i,j = ',ix_rec(irec),iy_rec(irec)
print *
enddo
endif
! check the Courant stability condition for the explicit time scheme
! R. Courant et K. O. Friedrichs et H. Lewy (1928)
Courant_number = cp * dsqrt(taumax)* DELTAT * sqrt(1.d0/DELTAX**2 + 1.d0/DELTAY**2 + 1.d0/DELTAZ**2)
if (rank == rank_cut_plane) then
print *,'Courant number is ',Courant_number
print *,'Vpmax=',cp*dsqrt(taumax)
endif
if (Courant_number > 1.d0) stop 'time step is too large, simulation will be unstable'
print *, "Number of points per wavelength =",cs*dsqrt(taumin)/(2.5d0*f0)/DELTAX,'Vsmin=',cs*dsqrt(taumin)
! erase main arrays
vx(:,:,:) = ZERO
vy(:,:,:) = ZERO
vz(:,:,:) = ZERO
sigmaxy(:,:,:) = ZERO
sigmayy(:,:,:) = ZERO
sigmazz(:,:,:) = ZERO
sigmaxz(:,:,:) = ZERO
sigmazz(:,:,:) = ZERO
sigmayz(:,:,:) = ZERO
e1(:,:,:,:) = ZERO
e11(:,:,:,:) = ZERO
e12(:,:,:,:) = ZERO
e13(:,:,:,:) = ZERO
e23(:,:,:,:) = ZERO
e22(:,:,:,:) = ZERO
! PML
memory_dvx_dx(:,:,:) = ZERO
memory_dvx_dy(:,:,:) = ZERO
memory_dvx_dz(:,:,:) = ZERO
memory_dvy_dx(:,:,:) = ZERO
memory_dvy_dy(:,:,:) = ZERO
memory_dvy_dz(:,:,:) = ZERO
memory_dvz_dx(:,:,:) = ZERO
memory_dvz_dy(:,:,:) = ZERO
memory_dvz_dz(:,:,:) = ZERO
memory_dsigmaxx_dx(:,:,:) = ZERO
memory_dsigmayy_dy(:,:,:) = ZERO
memory_dsigmazz_dz(:,:,:) = ZERO
memory_dsigmaxy_dx(:,:,:) = ZERO
memory_dsigmaxy_dy(:,:,:) = ZERO
memory_dsigmaxz_dx(:,:,:) = ZERO
memory_dsigmaxz_dz(:,:,:) = ZERO
memory_dsigmayz_dy(:,:,:) = ZERO
memory_dsigmayz_dz(:,:,:) = ZERO
! erase seismograms
sisvx(:,:) = ZERO
sisvy(:,:) = ZERO
! initialize total energy
total_energy(:) = ZERO
total_energy_kinetic(:) = ZERO
total_energy_potential(:) = ZERO
call date_and_time(datein,timein,zone,time_values)
! time_values(3): day of the month
! time_values(5): hour of the day
! time_values(6): minutes of the hour
! time_values(7): seconds of the minute
! time_values(8): milliseconds of the second
! this fails if we cross the end of the month
time_start = 86400.d0*time_values(3) + 3600.d0*time_values(5) + &
60.d0*time_values(6) + time_values(7) + time_values(8) / 1000.d0
!---
! we receive from the process on the left, and send to the process on the right
sender_right_shift = rank - 1
receiver_right_shift = rank + 1
! if we are the first process, there is no neighbor on the left
if (rank == 0) sender_right_shift = MPI_PROC_NULL
! if we are the last process, there is no neighbor on the right
if (rank == nb_procs - 1) receiver_right_shift = MPI_PROC_NULL
!---
! we receive from the process on the right, and send to the process on the left
sender_left_shift = rank + 1
receiver_left_shift = rank - 1
! if we are the first process, there is no neighbor on the left
if (rank == 0) receiver_left_shift = MPI_PROC_NULL
! if we are the last process, there is no neighbor on the right
if (rank == nb_procs - 1) sender_left_shift = MPI_PROC_NULL
k2begin = 1
if (rank == 0) k2begin = 2
kminus1end = NZ_LOCAL
if (rank == nb_procs - 1) kminus1end = NZ_LOCAL - 1
!---
!--- beginning of time loop
!---
do it = 1,NSTEP
if (rank == rank_cut_plane .and. mod(it,20) == 0) print *,'it = ',it
!----------------------
! compute stress sigma
!----------------------
! vx(k+1), left shift
call MPI_SENDRECV(vx(:,:,1:2),number_of_values,MPI_DOUBLE_PRECISION, &
receiver_left_shift,message_tag,vx(:,:,NZ_LOCAL+1:NZ_LOCAL+2),number_of_values, &
MPI_DOUBLE_PRECISION,sender_left_shift,message_tag,MPI_COMM_WORLD,message_status,code)
! vy(k+1), left shift
call MPI_SENDRECV(vy(:,:,1:2),number_of_values,MPI_DOUBLE_PRECISION, &
receiver_left_shift,message_tag,vy(:,:,NZ_LOCAL+1:NZ_LOCAL+2),number_of_values, &
MPI_DOUBLE_PRECISION,sender_left_shift,message_tag,MPI_COMM_WORLD,message_status,code)
! vz(k-1), right shift
call MPI_SENDRECV(vz(:,:,NZ_LOCAL-1:NZ_LOCAL),number_of_values,MPI_DOUBLE_PRECISION, &
receiver_right_shift,message_tag,vz(:,:,-1:0),number_of_values, &
MPI_DOUBLE_PRECISION,sender_right_shift,message_tag,MPI_COMM_WORLD,message_status,code)
do k=k2begin,NZ_LOCAL
kglobal = k + offset_k
do j=2,NY
do i=1,NX-1
mul_relaxed = mu
lambdal_relaxed = lambda
lambdalplus2mul_relaxed = lambdal_relaxed + TWO*mul_relaxed
lambdal_unrelaxed = (lambdal_relaxed + 2.d0/DIM*mul_relaxed) * Mu_nu1 - 2.d0/DIM*mul_relaxed * Mu_nu2
mul_unrelaxed = mul_relaxed * Mu_nu2
lambdalplus2mul_unrelaxed = lambdal_unrelaxed + TWO*mul_unrelaxed
value_dvx_dx = (27.d0*vx(i+1,j,k)-27.d0*vx(i,j,k)-vx(i+2,j,k)+vx(i-1,j,k)) * ONE_OVER_DELTAX/24.d0
value_dvy_dy = (27.d0*vy(i,j,k)-27.d0*vy(i,j-1,k)-vy(i,j+1,k)+vy(i,j-2,k)) * ONE_OVER_DELTAY/24.d0
value_dvz_dz = (27.d0*vz(i,j,k)-27.d0*vz(i,j,k-1)-vz(i,j,k+1)+vz(i,j,k-2)) * ONE_OVER_DELTAZ/24.d0
memory_dvx_dx(i,j,k) = b_x_half(i) * memory_dvx_dx(i,j,k) + a_x_half(i) * value_dvx_dx
memory_dvy_dy(i,j,k) = b_y(j) * memory_dvy_dy(i,j,k) + a_y(j) * value_dvy_dy
memory_dvz_dz(i,j,k) = b_z(kglobal) * memory_dvz_dz(i,j,k) + a_z(kglobal) * value_dvz_dz
duxdx = value_dvx_dx / K_x_half(i) + memory_dvx_dx(i,j,k)
duydy = value_dvy_dy / K_y(j) + memory_dvy_dy(i,j,k)
duzdz = value_dvz_dz / K_z(kglobal) + memory_dvz_dz(i,j,k)