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1c1< c******************************************************************************---> *******************************************************************************3,4c3,5< subroutine makeray(nx,ny,nz,fx,fy,fz,dxv,dyv,dzv,vel,vxx,vxy,vxz,< 1 vyy,vyz,vzz,x0,y0,z0,a0,azh,amin,amax,nr,nt,dt,---> subroutine makeray(nx,ny,nz,fx,fy,fz,dxv,dyv,dzv,vel,vxx,vxy,> 1 vxz,vyy,vyz,vzz,x0,y0,z0,a0,azh,amin,amax,nr,nt,dt,> 5 vg,vo,del,eps,axa,aya,nag,ndel,neps,dcg,ddel,deps,fdel,feps,7,29c8< 4 rq211,rq212,rq221,rq222,rv,rdvdx,rdvdy,rdvdz,nrs,< 5 map,v,dvdx,dvdy,dvdz,uxx,uxy,uxz,uyy,uyz,uzz,tzt,< 6 x,y,z,px,py,pz,e1x,e1y,e1z,e2x,e2y,e2z,< 7 p111,p112,p121,p122,q111,q112,< 8 q121,q122,p211,p212,p221,p222,< 9 q211,q212,q221,q222,dx,dy,dz,< a dpx,dpy,dpz,de1x,de1y,de1z,de2x,< b de2y,de2z,dp111,dp112,dp121,< c dp122,dq111,dq112,dq121,dq122,< d dp211,dp212,dp221,dp222,dq211,dq212,< e dq221,dq222,xt,yt,zt,pxt,pyt,pzt,< f e1xt,e1yt,e1zt,e2xt,e2yt,e2zt,< g p111t,p112t,p121t,p122t,< h q111t,q112t,q121t,q122t,p211t,< i p212t,p221t,p222t,q211t,< j q212t,q221t,q222t,dxt,dyt,< k dzt,dpxt,dpyt,dpzt,de1xt,< l de1yt,de1zt,de2xt,de2yt,de2zt,< m dp111t,dp112t,dp121t,dp122t,< n dq111t,dq112t,dq121t,dq122t,< o dp211t,dp212t,dp221t,dp222t,< p dq211t,dq212t,dq221t,dq222t,n1)< ---> 4 rq211,rq212,rq221,rq222,rv,rdvdx,rdvdy,rdvdz,rdt,nrs)43,45c22,24< c******************************************************************************< c* Trace rays for uniformly sampled vel(nz,ny,nx).< c******************************************************************************---> ******************************************************************************> c Trace rays for uniformly sampled v(x,y,z).> ******************************************************************************49d27< c nz number of z samples of velocity52a31> c nz number of z samples of velocity55a35> c vel sampled velocity65,67c45,46< c measured from y axis < c amin lower limit of emergence polar angle < c amax upper limit of emergence polar angle ---> c amin lower limit of emergence angle measured from z-axis> c amax upper limit of emergence angle measured from z-axis71,72c50,66< c < c****************************************************************************---> > c additional input variables for TI medium > c vg table of normalized group velocity --- array(nag,neps,ndel)> c nag number of group angle samples in the table > c neps number of epsilon samples in the table > c ndel number of delta samples in the table > c dcg sampling interval of cosin of group angle in the table > c deps sampling interval of epsilon in the table > c ddel sampling interval of delta in the table > c feps first sample of epsilon in the table > c fdel first sample of delta in the table > c vo sampled array(nz,ny,nx) of vertical velocity> c del sampled array(nz,ny,nx) of delta> c eps sampled array(nz,ny,nx) of epsilon> c axa sampled array(nz,ny,nx) of x-directivity of symmetric axis> c aya sampled array(nz,ny,nx) of y-directivity of symmetric axis> ******************************************************************************85c79,80< cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc---> c rdt residual traveltime due to anisotropy> ******************************************************************************90c85< c****************************************************************************---> *****************************************************************************/92,101c87,93< integer nrs(nr) < real vel(nz*ny*nx),vxx(nz*ny*nx),vxy(nz*ny*nx),vxz(nz*ny*nx),< 1 vyy(nz*ny*nx),vyz(nz*ny*nx),vzz(nz*ny*nx),< 2 a0(nr),azh(nr),rx(nt*nr),ry(nt*nr),rz(nt*nr),rpx(nt*nr),< 3 rpy(nt*nr),rpz(nt*nr),re1x(nt*nr),re1y(nt*nr),< 4 re1z(nt*nr),re2x(nt*nr),re2y(nt*nr),re2z(nt*nr),< 5 rq111(nt*nr),rq112(nt*nr),rq121(nt*nr),rq122(nt*nr),< 6 rp211(nt*nr),rp212(nt*nr),rp221(nt*nr),rp222(nt*nr),< 7 rq211(nt*nr),rq212(nt*nr),rq221(nt*nr),rq222(nt*nr),< 8 rv(nt*nr),rdvdx(nt*nr),rdvdy(nt*nr),rdvdz(nt*nr)---> integer nrs(*) > real vel(*),vxx(*),vxy(*),vxz(*),vyy(*),vyz(*),vzz(*),> 1 a0(*),azh(*),rx(*),ry(*),rz(*),rpx(*),rpy(*),rpz(*),> 2 re1x(*),re1y(*),re1z(*),re2x(*),re2y(*),re2z(*),> 3 rq111(*),rq112(*),rq121(*),rq122(*),rp211(*),rp212(*),> 4 rp221(*),rp222(*),rq211(*),rq212(*),rq221(*),rq222(*),> 5 rv(*),rdvdx(*),rdvdy(*),rdvdz(*)109,110c101< cccc parameter (n1=128)< integer n1---> parameter (n1=128)137,141c128,132< real fxr,lxt,fyr,lyr< < < cc call msgsci(" makeray n1= ",n1)< cc call msgsci(" makeray nr= ",nr)---> c additional variabels for anisotropy and perturbation> real vg(*),vo(*),del(*),eps(*),axa(*),aya(*),rdt(*) > real axa0(n1),aya0(n1),vg0(n1),> 1 vo0(n1),del0(n1),eps0(n1),cg0(n1)> 168d158< ccc call msgsci(" loop 5 nr= ",nr)204d193< ccc call msgsci(" loop 10 nr= ",nr)213d201< ccc call msgsci(" loop 20 nr= ",nr)240d227< ccc call msgsci(" loop 50 nr= ",nr)270a258> rdt(ir) = 0.272,273d259< < ccc call msgsci(" after loop 50 nr= ",nr)290,294d275< c boundary tolerance< fxr = fx - 0.001*dxv< lxr = lx + 0.001*dxv< fyr = fy - 0.001*dyv< lyr = ly + 0.001*dyv296,304d276< c call msgscf("tzmin=",tzmin)< c call msgscf("tzmax=",tzmax)< c call msgscf("fx=",fx)< c call msgscf("lx=",lx)< c call msgscf("fy=",fy)< c call msgscf("ly=",ly)< c call msgscf("fz=",fz)< c call msgscf("lz=",lz)< 311,317d282< < cccc round up to the boudaries if x,y,z are very close < if(x(ir).lt.fx .and. x(ir).gt.fxr) x(ir) = fx< if(x(ir).gt.lx .and. x(ir).lt.lxr) x(ir) = lx< if(y(ir).lt.fy .and. y(ir).gt.fxr) y(ir) = fy< if(y(ir).gt.ly .and. y(ir).lt.lyr) y(ir) = ly< 322,331d286< < c if(x(ir).lt.fx) call msgscf("x=",x(ir))< c if(x(ir).gt.lx) call msgscf("x=",x(ir))< c if(y(ir).lt.fy) call msgscf("y=",y(ir))< c if(y(ir).gt.ly) call msgscf("y=",y(ir))< c if(z(ir).lt.fz) call msgscf("z=",z(ir))< c if(z(ir).gt.lz) call msgscf("z=",z(ir))< c if(tzt(ir).lt.tzmin) call msgscf("tzt=",tzt(ir))< c if(tzt(ir).gt.tzmax) call msgscf("tzt=",tzt(ir))< 517a473,476> > c interpolate anisotropic parameters> call anip3Interp(nx,ny,nz,fx,fy,fz,dxv,dyv,dzv,> 1 vo,del,eps,axa,aya,x,y,z,nr,vo0,del0,eps0,axa0,aya0)518a478,489> c compute group angle> > do 490 ir=1,nr> cg0(ir) = v(ir)*(px(ir)*axa0(ir)+py(ir)*aya0(ir)+pz(ir)> 1 *sqrt(1-axa0(ir)*axa0(ir)-aya0(ir)*aya0(ir)))> cg0(ir) = abs(cg0(ir))> 490 end do> > c look up group velocity table> call vg3Interp(ndel,neps,nag,fdel,feps,1.0,ddel,deps,-dcg,> 1 vg,del0,eps0,cg0,nr,vg0)> 549a521,523> c calculate traveltime perturbation due to anisotropy> rdt(it*nrsave+jr) = (v(ir)/(vg0(ir)*vo0(ir))-1.0)*dt>
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