C ************************** C * PDE2D 9.5 MAIN PROGRAM * C ************************** C *** 3D PROBLEM SOLVED *** C############################################################################## C Is double precision mode to be used? Double precision is recommended. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If double precision mode is used, variables and functions assigned +# C + names beginning with a letter in the range A-H or O-Z will be DOUBLE +# C + PRECISION, and you should use double precision constants and FORTRAN +# C + expressions throughout; otherwise such variables and functions will +# C + be of type REAL. In either case, variables and functions assigned +# C + names beginning with I,J,K,L,M or N will be of INTEGER type. +# C + +# C + It is possible to convert a single precision PDE2D program to double +# C + precision after it has been created, using an editor. Just change +# C + all occurrences of "real" to "double precision" +# C + " tdp" to "dtdp" (note leading blank) +# C + Any user-written code or routines must be converted "by hand", of +# C + course. To convert from double to single, reverse the changes. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## implicit double precision (a-h,o-z) parameter (neqnmx= 99) C############################################################################## C NP1GRID = number of P1-grid lines # C############################################################################## PARAMETER (NP1GRID = 13) C############################################################################## C NP2GRID = number of P2-grid lines # C############################################################################## PARAMETER (NP2GRID = 13) C############################################################################## C NP3GRID = number of P3-grid lines # C############################################################################## PARAMETER (NP3GRID = 8) C############################################################################## C How many differential equations (NEQN) are there in your problem? # C############################################################################## PARAMETER (NEQN = 3) C DIMENSIONS OF WORK ARRAYS C SET TO 1 FOR AUTOMATIC ALLOCATION PARAMETER (IRWK8Z= 1) PARAMETER (IIWK8Z= 1) PARAMETER (NXP8Z=41,NYP8Z=41,NZP8Z=41,KDEG8Z=1) C############################################################################## C The solution is normally saved on an NP1+1 by NP2+1 by NP3+1 # C rectangular grid of points, # C P1 = P1A + I*(P1B-P1A)/NP1, I = 0,...,NP1 # C P2 = P2A + J*(P2B-P2A)/NP2, J = 0,...,NP2 # C P3 = P3A + K*(P3B-P3A)/NP3, K = 0,...,NP3 # C Enter values for NP1, NP2 and NP3. Suggested values: NP1=NP2=NP3=16. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If you want to save the solution at an arbitrary user-specified set +# C + of points, set NP2=NP3=0 and NP1+1=number of points. In this case +# C + you can request tabular output, but no plots can be made. +# C + +# C + If you set NEAR8Z=1 in the main program, the values saved at each +# C + output point will actually be the solution as evaluated at a nearby +# C + collocation point. For most problems this obviously will produce +# C + less accurate output or plots, but for certain (rare) problems, a +# C + solution component may be much less noisy when plotted only at +# C + collocation points. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## PARAMETER (NP1 = 16) PARAMETER (NP2 = 16) PARAMETER (NP3 = 7) PARAMETER (NSAVE = 1) common/parm8z/ pi dimension p1grid(np1grid),p2grid(np2grid),p3grid(np3grid),p1out8z( &0:np1,0:np2,0:np3),p2out8z(0:np1,0:np2,0:np3),p3out8z(0:np1,0:np2, &0:np3),p1cross(100),p2cross(100),p3cross(100),tout8z(0:nsave) C dimension xres8z(nxp8z),yres8z(nyp8z),zres8z(nzp8z), C & ures8z(neqn,nxp8z,nyp8z,nzp8z) allocatable iwrk8z(:),rwrk8z(:) C dimension iwrk8z(iiwk8z),rwrk8z(irwk8z) character*40 title logical linear,crankn,noupdt,nodist,fillin,evcmpx,adapt,plot,lsqfi &t,fdiff,solid,econ8z,ncon8z,restrt,gridid common/dtdp14/ sint8z(20),bint8z(20),slim8z(20),blim8z(20) common/dtdp15/ evlr8z,ev0r,evli8z,ev0i,evcmpx common/dtdp16/ p8z,evr8z(50),evi8z(50) common/dtdp19/ toler(neqnmx),adapt common/dtdp30/ econ8z,ncon8z common/dtdp45/ perdc(neqnmx) common/dtdp46/ eps8z,cgtl8z,npmx8z,itype,near8z common/dtdp52/ nxa8z,nya8z,nza8z,kd8z common/dtdp53/ work8z(nxp8z*nyp8z*nzp8z+9) common/dtdp64/ amin8z(4*neqnmx),amax8z(4*neqnmx) common/dtdp77/ nx18z,ny18z,nz18z,p1a,p1b,p2a,p2b,p3a,p3b,uout(0:np &1,0:np2,0:np3,4,neqn,0:nsave) pi = 4.0*atan(1.d0) nxa8z = nxp8z nya8z = nyp8z nza8z = nzp8z nx18z = np1+1 ny18z = np2+1 nz18z = np3+1 kd8z = kdeg8z C############################################################################## C If you don't want to read the FINE PRINT, default NPROB. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If you want to solve several similar problems in the same run, set +# C + NPROB equal to the number of problems you want to solve. Then NPROB +# C + loops through the main program will be done, with IPROB=1,...,NPROB, +# C + and you can make the problem parameters vary with IPROB. NPROB +# C + defaults to 1. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## NPROB = 1 do 78755 iprob=1,nprob C############################################################################## C PDE2D solves the time-dependent system (note: U,F,G,U0 may be vectors, # C C,RHO may be matrices): # C # C C(X,Y,Z,T,U,Ux,Uy,Uz)*d(U)/dT = # C F(X,Y,Z,T,U,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz) # C # C or the steady-state system: # C # C F(X,Y,Z,U,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz) = 0 # C # C or the linear and homogeneous eigenvalue system: # C # C F(X,Y,Z,U,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz) = lambda*RHO(X,Y,Z)*U # C # C with boundary conditions: # C # C G(X,Y,Z,[T],U,Ux,Uy,Uz) = 0 # C (periodic boundary conditions are also permitted) # C # C For time-dependent problems there are also initial conditions: # C # C U = U0(X,Y,Z) at T=T0 # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If your PDEs involve the solution at points other than (P1,P2,P3), +# C + the function +# C + (D)OLDSOL3(IDER,IEQ,PP1,PP2,PP3,KDEG) +# C + will interpolate (using interpolation of degree KDEG=1,2 or 3) to +# C + (PP1,PP2,PP3) the function saved in UOUT(*,*,*,IDER,IEQ,ISET) on the +# C + last time step or iteration (ISET) for which it has been saved. +# C + Thus, for example, if IDER=1, this will return the latest value of +# C + component IEQ of the solution at (PP1,PP2,PP3), assuming this has +# C + not been modified using UPRINT... If your equations involve +# C + integrals of the solution, for example, you can use (D)OLDSOL3 to +# C + approximate these using the solution from the last time step or +# C + iteration. +# C + +# C + CAUTION: For a steady-state or eigenvalue problem, you must reset +# C + NOUT=1 if you want to save the solution each iteration. +# C ++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++# C + A system of NEQN complex partial differential equations must be +# C + written as a system of 2*NEQN real equations, by separating the +# C + equations into their real and imaginary parts. However, note that +# C + the complex arithmetic abilities of FORTRAN can be used to simplify +# C + this separation. For example, the complex PDE: +# C + I*(Uxx+Uyy+Uzz) - 1/(1+U**10) = 0, where U = UR + UI*I +# C + would be difficult to split up analytically, but using FORTRAN +# C + expressions it is easy: +# C + F1 = -(UIxx+UIyy+UIzz) - REAL(1.0/(1.0+CMPLX(UR,UI)**10)) +# C + F2 = (URxx+URyy+URzz) - AIMAG(1.0/(1.0+CMPLX(UR,UI)**10)) +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C You may now define global parameters, which may be referenced in any # C of the "FORTRAN expressions" you input throughout the rest of this # C interactive session. You will be prompted alternately for parameter # C names and their values; enter a blank name when you are finished. # C # C Parameter names are valid FORTRAN variable names, starting in # C column 1. Thus each name consists of 1 to 6 alphanumeric characters, # C the first of which must be a letter. If the first letter is in the # C range I-N, the parameter must be an integer. # C # C Parameter values are either FORTRAN constants or FORTRAN expressions # C involving only constants and global parameters defined on earlier # C lines. They may also be functions of the problem number IPROB, if # C you are solving several similar problems in one run (NPROB > 1). Note # C that you are defining global CONSTANTS, not functions; e.g., parameter # C values may not reference any of the independent or dependent variables # C of your problem. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If you define other parameters here later, using an editor, you must +# C + add them to COMMON block /PARM8Z/ everywhere this block appears, if +# C + they are to be "global" parameters. +# C + +# C + The variable PI is already included as a global parameter, with an +# C + accurate value 3.14159... +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## C############################################################################## C A collocation finite element method is used, with tri-cubic Hermite # C basis functions on the elements (small boxes) defined by the grid # C points: # C P1GRID(1),...,P1GRID(NP1GRID) # C P2GRID(1),...,P2GRID(NP2GRID) # C P3GRID(1),...,P3GRID(NP3GRID) # C You will first be prompted for NP1GRID, the number of P1-grid points, # C then for P1GRID(1),...,P1GRID(NP1GRID). Any points defaulted will be # C uniformly spaced between the points you define; the first and last # C points cannot be defaulted. Then you will be prompted similarly # C for the number and values of the P2 and P3-grid points. The limits # C on the parameters are then: # C P1GRID(1) < P1 < P1GRID(NP1GRID) # C P2GRID(1) < P2 < P2GRID(NP2GRID) # C P3GRID(1) < P3 < P3GRID(NP3GRID) # C # C############################################################################## call dtdpwx(p1grid,np1grid,0) call dtdpwx(p2grid,np2grid,0) call dtdpwx(p3grid,np3grid,0) C P1GRID DEFINED P1GRID(1) = & 0 P1GRID(NP1GRID) = & 2*pi C P2GRID DEFINED P2GRID(1) = & 0 P2GRID(NP2GRID) = & 2*pi C P3GRID DEFINED P3GRID(1) = & 1 P3GRID(NP3GRID) = & 4 call dtdpwx(p1grid,np1grid,1) call dtdpwx(p2grid,np2grid,1) call dtdpwx(p3grid,np3grid,1) C############################################################################## C If you don't want to read the FINE PRINT, enter ISOLVE = 1. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + The following linear system solvers are available: +# C + +# C + 1. Sparse direct method +# C + Harwell Library routine MA27 (used by permission) is +# C + used to solve the (positive definite) "normal" +# C + equations A**T*A*x = A**T*b. The normal equations, +# C + which are essentially the equations which would result +# C + if a least squares finite element method were used +# C + instead of a collocation method, are substantially +# C + more ill-conditioned than the original system Ax = b, +# C + so it may be important to use high precision if this +# C + option is chosen. +# C + 2. Frontal method +# C + This is an out-of-core band solver. If you want to +# C + override the default number of rows in the buffer (11),+# C + set a new value for NPMX8Z in the main program. +# C + 3. Jacobi conjugate gradient iterative method +# C + A preconditioned conjugate gradient iterative method +# C + is used to solve the (positive definite) normal +# C + equations. High precision is also important if this +# C + option is chosen. (This solver is MPI-enhanced, if +# C + MPI is available.) If you want to override the +# C + default convergence tolerance, set a new relative +# C + tolerance CGTL8Z in the main program. +# C + 4. Local solver (normal equations) +# C + 5. Local solver (original equations) +# C + Choose these options ONLY if alterative linear system +# C + solvers have been installed locally. See subroutines +# C + (D)TD3M, (D)TD3N in file (d)subs.f for instructions +# C + on how to add local solvers. +# C + 6. MPI-based parallel band solver +# C + This is a parallel solver which runs efficiently on +# C + multiple processor machines, under MPI. It is a +# C + band solver, with the matrix distributed over the +# C + available processors. Choose this option ONLY if the +# C + solver has been activated locally. See subroutine +# C + (D)TD3O in file (d)subs.f for instructions on how to +# C + activate this solver and the MPI-enhancements to the +# C + conjugate gradient solver. +# C + +# C + Enter ISOLVE = 1,2,3,4,5 or 6 to select a linear system solver. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## ISOLVE = 2 C *******STEADY-STATE PROBLEM itype = 1 t0 = 0.0 dt = 1.0 crankn = .false. noupdt = .false. C############################################################################## C Is this a linear problem? ("linear" means all differential equations # C and all boundary conditions are linear). If you aren't sure, it is # C safer to answer "no". # C############################################################################## LINEAR = .FALSE. C############################################################################## C Give an upper limit on the number of Newton's method iterations # C (NSTEPS) to be allowed for this nonlinear problem. NSTEPS defaults # C to 15. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + The iteration will stop if convergence occurs before the upper +# C + limit has been reached. In the FORTRAN program created by the +# C + preprocessor, NCON8Z will be .TRUE. if Newton's method has converged.+# C + +# C + For highly non-linear problems you may want to construct a one- +# C + parameter family of problems using the variable T, such that for +# C + T=1 the problems is easy (e.g. linear) and for T > N (N is less +# C + NSTEPS), the problem reduces to the original highly nonlinear +# C + problem. For example, the nonlinear term(s) may be multiplied by +# C + MIN(1.0,(T-1.0)/N). +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## NSTEPS = 10 FDIFF = .TRUE. C############################################################################## C You may calculate one or more integrals (over the entire region) of # C some functions of the solution and its derivatives. How many integrals # C (NINT), if any, do you want to calculate? # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + In the FORTRAN program created by the preprocessor, the computed +# C + values of the integrals will be returned in the vector SINT8Z. If +# C + several iterations or time steps are done, only the last computed +# C + values are saved in SINT8Z (all values are printed). +# C + +# C + A limiting value, SLIM8Z(I), for the I-th integral can be set +# C + below in the main program. The computations will then stop +# C + gracefully whenever SINT8Z(I) > SLIM8Z(I), for any I=1...NINT. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## NINT = 1 C############################################################################## C You may calculate one or more boundary integrals (over the entire # C boundary) of some functions of the solution and its derivatives. How # C many boundary integrals (NBINT), if any, do you want to calculate? # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + In the FORTRAN program created by the preprocessor, the computed +# C + values of the integrals will be returned in the vector BINT8Z. If +# C + several iterations or time steps are done, only the last computed +# C + values are saved in BINT8Z (all values are printed). +# C + +# C + A limiting value, BLIM8Z(I), for the I-th boundary integral can be +# C + set below in the main program. The computations will then stop +# C + gracefully whenever BINT8Z(I) > BLIM8Z(I), for any I=1...NBINT. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## NBINT = 0 lsqfit = .false. C############################################################################## C If you don't want to read the FINE PRINT, enter 'no'. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + Do you want to read the initial conditions from the restart file, +# C + if it exists (and use the conditions supplied above if it does not +# C + exist)? +# C + +# C + If so, PDE2D will dump the final solution at the end of each run +# C + into a restart file "pde2d.res". Thus the usual procedure for +# C + using this dump/restart option is to make sure there is no restart +# C + file in your directory left over from a previous job, then the +# C + first time you run this job, the initial conditions supplied above +# C + will be used, but on the second and subsequent runs the restart file +# C + from the previous run will be used to define the initial conditions. +# C + +# C + You can do all the "runs" in one program, by setting NPROB > 1. +# C + Each pass through the DO loop, T0,TF,NSTEPS and possibly other +# C + parameters may be varied, by making them functions of IPROB. +# C + +# C + If the 2D or 3D collocation method is used, the coordinate +# C + transformation should not change between dump and restart. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## RESTRT = .FALSE. C GRIDID = .FALSE. IF FINITE ELEMENT GRID CHANGES BETWEEN DUMP, RESTART GRIDID = .TRUE. C############################################################################## C If you do not have any periodic boundary conditions, enter IPERDC=0. # C # C Enter IPERDC=1 for periodic conditions at P1 = P1GRID(1),P1GRID(NP1GRID)# C IPERDC=2 for periodic conditions at P2 = P2GRID(1),P2GRID(NP2GRID)# C IPERDC=3 for periodic conditions at P3 = P3GRID(1),P3GRID(NP3GRID)# C IPERDC=4 for periodic conditions on both P1 and P2 # C IPERDC=5 for periodic conditions on both P1 and P3 # C IPERDC=6 for periodic conditions on both P2 and P3 # C IPERDC=7 for periodic conditions on P1, P2 and P3. # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + When periodic boundary conditions are selected, they apply to all +# C + variables by default. To turn off periodic boundary conditions on +# C + the I-th variable, set PERDC(I) to 0 (or another appropriate value +# C + of IPERDC) below in the main program and set the desired boundary +# C + conditions in subroutine GB8Z, "by hand". +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## IPERDC = 4 C############################################################################## C The solution is saved on an NP1+1 by NP2+1 by NP3+1 rectangular grid # C covering the box (P1A,P1B) x (P2A,P2B) x (P3A,P3B). Enter values for # C P1A,P1B,P2A,P2B,P3A,P3B. These variables are usually defaulted. # C # C The defaults are P1A = P1GRID(1), P1B = P1GRID(NP1GRID) # C P2A = P2GRID(1), P2B = P2GRID(NP2GRID) # C P3A = P3GRID(1), P3B = P3GRID(NP3GRID) # C # C############################################################################## C defaults for p1a,p1b,p2a,p2b,p3a,p3b p1a = p1grid(1) p1b = p1grid(np1grid) p2a = p2grid(1) p2b = p2grid(np2grid) p3a = p3grid(1) p3b = p3grid(np3grid) C DEFINE P1A,P1B,P2A,P2B,P3A,P3B IMMEDIATELY BELOW: call dtdpx3(np1,np2,np3,p1a,p1b,p2a,p2b,p3a,p3b,hp18z,hp28z,hp38z, &p1out8z,p2out8z,p3out8z,npts8z) C SOLUTION SAVED EVERY NOUT ITERATIONS NOUT = NSTEPS call dtdpqx(np1grid,np2grid,np3grid,isolve,neqn,ii8z,ir8z,iperdc) if (iiwk8z.gt.1) ii8z = iiwk8z if (irwk8z.gt.1) ir8z = irwk8z C *******allocate workspace allocate (iwrk8z(ii8z),rwrk8z(ir8z)) C *******DRAW GRID LINES? PLOT = .FALSE. C *******call pde solver call dtdp3x(p1grid, p2grid, p3grid, np1grid, np2grid, np3grid, neq &n, p1out8z, p2out8z, p3out8z, uout, tout8z, npts8z, t0, dt, nsteps &, nout, nsave, crankn, noupdt, itype, linear, isolve, rwrk8z, ir8z &, iwrk8z, ii8z, iperdc, plot, lsqfit, fdiff, nint, nbint, restrt, &gridid) deallocate (iwrk8z,rwrk8z) C *******UNCOMMENT TO POSTPROCESS ONLY IF CONVERGED C IF (.NOT.NCON8Z) GO TO 78755 C *******read from restart file to array ures8z C call dtdpr3(1,xres8z,nxp8z,yres8z,nyp8z,zres8z,nzp8z,ures8z,neqn) C *******write array ures8z back to restart file C call dtdpr3(2,xres8z,nxp8z,yres8z,nyp8z,zres8z,nzp8z,ures8z,neqn) C *******call user-written postprocessor call postpr(tout8z,nsave,p1out8z,p2out8z,p3out8z,np1,np2,np3,uout, &neqn,p1grid,p2grid,p3grid,np1grid,np2grid,np3grid) C *******CROSS-SECTION VECTOR PLOTS C P1 = CONSTANT CROSS-SECTIONS ics8z = 1 C############################################################################## C Plots of the variable or vector as a function of P2 and P3 will be # C made, at the output grid P1-points closest to # C P1 = P1CROSS(1),...,P1CROSS(NP1VALS) # C # C Enter values for NP1VALS and P1CROSS(1),...,P1CROSS(NP1VALS). # C############################################################################## NP1VALS = 2 P1CROSS(1) = & 0 P1CROSS(2) = & pi/2. C############################################################################## C If your region is rectangular, enter ITPLOT=0, and you need not read # C the FINE PRINT. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + Enter: +# C + ITPLOT = 0 if you want a rectangular cross-section to be drawn, +# C + with axes P2 and P3 (recommended when ITRANS=0,1,-1,2, +# C + or -2) +# C + ITPLOT = 1 if you want a polar cross-section to be drawn, with +# C + P2=radius, P3=angle (axes A1=P2*COS(P3) and +# C + A2=P2*SIN(P3)). +# C + ITPLOT = -1 if you want a polar cross-section to be drawn, with +# C + P3=radius, P2=angle (axes A1=P3*COS(P2) and +# C + A2=P3*SIN(P2)). +# C + ITPLOT = 2 if the desired cross-section is neither rectangular +# C + nor polar, and you want to define the axes A1,A2 +# C + yourself. (Sometimes recommended when ITRANS=3,-3.) +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## ITPLOT = 2 ical8z = 1 C############################################################################## C If you don't want to read the FINE PRINT, default A1MIN,A1MAX,A2MIN, # C and A2MAX. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + By default, at each cross-section the limits (A1MIN,A1MAX) and +# C + (A2MIN,A2MAX) on the axes A1 and A2 are chosen so that the plot just +# C + fills the plot space. For a non-rectangular region, this means the +# C + scale may vary from cross-section to cross-section. Enter values +# C + for A1MIN,A1MAX,A2MIN,A2MAX here if you want to ensure a common +# C + scale for all cross-sections. (You must specify all four variables, +# C + or default all four.) +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## A1MIN = 0.0 A1MAX = 0.0 A2MIN = 0.0 A2MAX = 0.0 C############################################################################## C Enter values for IVAR1, IVAR2, IVAR3 to select the components Vr1,Vr2 # C and Vr3 of the vector to be plotted. # C IVAR1,IVAR2,IVAR3 = 1 means U (possibly as modified by UPRINT,...) # C 2 Ux # C 3 Uy # C 4 Uz # C 5 V # C 6 Vx # C 7 Vy # C 8 Vz # C 9 W # C 10 Wx # C 11 Wy # C 12 Wz # C # C A vector plot of the in-plane components (Vr1,Vr2) will be made, with a # C contour plot of the out-of-plane component Vr3 superimposed. # C # C Caution: If ITPLOT.NE.0, Vr1 and Vr2 are assumed to be the components # C of the in-plane vector in the directions of the NEW axes A1,A2. # C############################################################################## IVAR1 = 1 IVAR2 = 9 IVAR3 = 5 ivar1a8z = mod(ivar1-1,4)+1 ivar1b8z = (ivar1-1)/4+1 ivar2a8z = mod(ivar2-1,4)+1 ivar2b8z = (ivar2-1)/4+1 ivar3a8z = mod(ivar3-1,4)+1 ivar3b8z = (ivar3-1)/4+1 ISET1 = 1 ISET2 = NSAVE ISINC = 1 C############################################################################## C If you don't want to read the FINE PRINT, enter 'no'. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + Do you want to scale the axes on the plot so that the region is +# C + undistorted? Otherwise the axes will be scaled so that the figure +# C + approximately fills the plot space. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## NODIST = .FALSE. C a1mag = max(abs(amin8z(ivar1)),abs(amax8z(ivar1))) a2mag = max(abs(amin8z(ivar2)),abs(amax8z(ivar2))) C############################################################################## C For the purpose of scaling the arrows, the ranges of the two components # C of the vector are assumed to be (-VR1MAG,VR1MAG) and (-VR2MAG,VR2MAG). # C Enter values for VR1MAG and VR2MAG. VR1MAG and VR2MAG are often # C defaulted. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + By default, VR1MAG and VR2MAG are the maxima of the absolute values +# C + of the first and second components. For a common scaling, you may +# C + want to set VR1MAG=A1MAG, VR2MAG=A2MAG. A1MAG, A2MAG are the +# C + maxima of the absolute values over all output points and over all +# C + saved time steps or iterations. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## VR1MAG = A1MAG VR2MAG = A2MAG C a3low = amin8z(ivar3) a3high = amax8z(ivar3) C############################################################################## C Enter lower (VR3MIN) and upper (VR3MAX) bounds for the contour values # C for the third component of the vector. VR3MIN and VR3MAX are often # C defaulted. # C # C Contours will be drawn corresponding to the values # C # C VR3MIN + S*(VR3MAX-VR3MIN), for S=0.05,0.15,...0.95. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + By default, VR3MIN and VR3MAX are set to the minimum and maximum +# C + values of the variable to be plotted. For a common scaling, you may +# C + want to set VR3MIN=A3LOW, VR3MAX=A3HIGH. A3LOW and A3HIGH are the +# C + minimum and maximum values over all output points and over all saved +# C + time steps or iterations. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## VR3MIN = A3LOW VR3MAX = A3HIGH C############################################################################## C Enter a title, WITHOUT quotation marks. A maximum of 40 characters # C are allowed. The default is no title. # C############################################################################## TITLE = ' ' TITLE = 'Velocity Field ' call dtdprx(tout8z,nsave,iset1,iset2,isinc) do 78757 is8z=iset1,iset2,isinc do 78756 ixv8z=1,np1vals call dtdpzx(p1cross(ixv8z),p1a,p1b,np1,ix8z) call dtdplq(uout(0,0,0,ivar1a8z,ivar1b8z,is8z),uout(0,0,0,ivar2a8z &,ivar2b8z,is8z),uout(0,0,0,ivar3a8z,ivar3b8z,is8z),np1,np2,np3,p1a &,p1b,p2a,p2b,p3a,p3b,ics8z,ix8z,jy8z,kz8z,title,vr1mag,vr2mag,vr3m &in,vr3max,nodist,tout8z(is8z),a1min,a1max,a2min,a2max,itplot,ical8 &z) 78756 continue 78757 continue 78755 continue call endgks stop end subroutine tran8z(itrans,p1,p2,p3) implicit double precision (a-h,o-z) common /dtdp41/x,y,z,x1,x2,x3,y1,y2,y3,z1,z2,z3,x11,x21,x31,x12,x2 &2,x32,x13,x23,x33,y11,y21,y31,y12,y22,y32,y13,y23,y33,z11,z21,z31, &z12,z22,z32,z13,z23,z33 common/parm8z/ pi C############################################################################## C You can solve problems in your region only if you can describe it by # C X = X(P1,P2,P3) # C Y = Y(P1,P2,P3) # C Z = Z(P1,P2,P3) # C with constant limits on the parameters P1,P2,P3. If your region is # C rectangular, enter ITRANS=0 and the trivial parameterization # C X = P1 # C Y = P2 # C Z = P3 # C will be used. Otherwise, you need to read the FINE PRINT below. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If P1,P2,P3 represent cylindrical, spherical or other non-Cartesian +# C + coordinates, you can reference the Cartesian coordinates X,Y,Z +# C + and derivatives of your unknowns with respect to these coordinates, +# C + when you define your PDE coefficients, boundary conditions, and +# C + volume and boundary integrals, if you enter ITRANS .NE. 0. Enter: +# C + ITRANS = 1, if P1,P2,P3 are cylindrical coordinates, that is, if +# C + P1=R, P2=Theta, P3=Z, where X = R*cos(Theta) +# C + Y = R*sin(Theta) +# C + Z = Z +# C + ITRANS = -1, same as ITRANS=1, but P1=Theta, P2=R, P3=Z +# C + ITRANS = 2, if P1,P2,P3 are spherical coordinates, that is, if +# C + P1=Rho, P2=Phi, P3=Theta, where +# C + X = Rho*sin(Phi)*cos(Theta) +# C + Y = Rho*sin(Phi)*sin(Theta) +# C + Z = Rho*cos(Phi) +# C + (Theta is longitude, Phi is measured from north pole) +# C + ITRANS = -2, same as ITRANS=2, but P1=Rho, P2=Theta, P3=Phi +# C + ITRANS = 3, to define your own coordinate transformation. In this +# C + case, you will be prompted to define X,Y,Z and their +# C + first and second derivatives in terms of P1,P2,P3. +# C + Because of symmetry, you will not be prompted for all +# C + of the second derivatives. If you make a mistake in +# C + computing any of these derivatives, PDE2D will usually +# C + be able to issue a warning message. (X1 = dX/dP1, etc) +# C + ITRANS = -3, same as ITRANS=3, but you will only be prompted to +# C + define X,Y,Z; their first and second derivatives will +# C + be approximated using finite differences. +# C + When ITRANS = -3 or 3, the first derivatives of X,Y,Z must all be +# C + continuous. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## ITRANS = -3 X = & (5.0+p3*cos(p2))*cos(p1) Y = & (5.0+p3*cos(p2))*sin(p1) Z = & p3*sin(p2) return end subroutine pdes8z(yd8z,i8z,j8z,kint8z,p1,p2,p3,t,uu8z) implicit double precision (a-h,o-z) parameter (neqnmx= 99) C un8z(1,I),un8z(2,I),... hold the (rarely used) values C of UI,UI1,... from the previous iteration or time step common /dtdp5x/un8z(10,neqnmx) common /dtdp18/norm1,norm2,norm3 double precision norm1,norm2,norm3,normx,normy,normz dimension uu8z(10,neqnmx) common/parm8z/ pi U = uu8z(1, 1) U1 = uu8z(2, 1) U2 = uu8z(3, 1) U3 = uu8z(4, 1) U11= uu8z(5, 1) U22= uu8z(6, 1) U33= uu8z(7, 1) U12= uu8z(8, 1) U21= uu8z(8, 1) U13= uu8z(9, 1) U31= uu8z(9, 1) U23= uu8z(10, 1) U32= uu8z(10, 1) V = uu8z(1, 2) V1 = uu8z(2, 2) V2 = uu8z(3, 2) V3 = uu8z(4, 2) V11= uu8z(5, 2) V22= uu8z(6, 2) V33= uu8z(7, 2) V12= uu8z(8, 2) V21= uu8z(8, 2) V13= uu8z(9, 2) V31= uu8z(9, 2) V23= uu8z(10, 2) V32= uu8z(10, 2) W = uu8z(1, 3) W1 = uu8z(2, 3) W2 = uu8z(3, 3) W3 = uu8z(4, 3) W11= uu8z(5, 3) W22= uu8z(6, 3) W33= uu8z(7, 3) W12= uu8z(8, 3) W21= uu8z(8, 3) W13= uu8z(9, 3) W31= uu8z(9, 3) W23= uu8z(10, 3) W32= uu8z(10, 3) call dtdpcd(p1,p2,p3) call dtdpcb(p1,p2,p3,norm1,norm2,norm3,x,y,z,normx,normy,normz,3) call dtdpcc(p1,p2,p3, & U1,U2,U3,U11,U22,U33,U12,U13,U23, & x,y,z,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz, & Uyx,Uzx,Uzy,dvol,darea) Unorm = Ux*normx + Uy*normy + Uz*normz call dtdpcc(p1,p2,p3, & V1,V2,V3,V11,V22,V33,V12,V13,V23, & x,y,z,Vx,Vy,Vz,Vxx,Vyy,Vzz,Vxy,Vxz,Vyz, & Vyx,Vzx,Vzy,dvol,darea) Vnorm = Vx*normx + Vy*normy + Vz*normz call dtdpcc(p1,p2,p3, & W1,W2,W3,W11,W22,W33,W12,W13,W23, & x,y,z,Wx,Wy,Wz,Wxx,Wyy,Wzz,Wxy,Wxz,Wyz, & Wyx,Wzx,Wzy,dvol,darea) Wnorm = Wx*normx + Wy*normy + Wz*normz if (i8z.eq.0) then yd8z = 0.0 C############################################################################## C Enter FORTRAN expressions for the functions whose integrals are to be # C calculated and printed. They may be functions of # C # C X,Y,Z,U,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz # C V,Vx,Vy,Vz,Vxx,Vyy,Vzz,Vxy,Vxz,Vyz # C W,Wx,Wy,Wz,Wxx,Wyy,Wzz,Wxy,Wxz,Wyz # C and (if applicable) T # C # C The parameters P1,P2,P3 and derivatives with respect to these may also # C be referenced (U1 = dU/dP1, etc): # C U1,U2,U3,U11,U22,U33,U12,U13,U23 # C V1,V2,V3,V11,V22,V33,V12,V13,V23 # C W1,W2,W3,W11,W22,W33,W12,W13,W23 # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If you only want to integrate a function over part of the region, +# C + define that function to be zero in the rest of the region. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## C INTEGRAL DEFINED if (kint8z.eq. 1) yd8z = & abs(U)+abs(V)+abs(W) C############################################################################## C Enter FORTRAN expressions for the functions whose integrals are to be # C calculated and printed. They may be functions of # C # C X,Y,Z,U,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz # C V,Vx,Vy,Vz,Vxx,Vyy,Vzz,Vxy,Vxz,Vyz # C W,Wx,Wy,Wz,Wxx,Wyy,Wzz,Wxy,Wxz,Wyz # C and (if applicable) T # C # C The components (NORMx,NORMy,NORMz) of the unit outward normal vector # C may also be referenced. # C # C The parameters P1,P2,P3 and derivatives with respect to these may # C also be referenced: # C U1,U2,U3,U11,U22,U33,U12,U13,U23 # C V1,V2,V3,V11,V22,V33,V12,V13,V23 # C W1,W2,W3,W11,W22,W33,W12,W13,W23 # C You can also reference the normal derivatives Unorm,Vnorm,Wnorm. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If you only want to integrate a function over part of the boundary, +# C + define that function to be zero on the rest of the boundary. +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## C BND. INTEGRAL1 DEFINED C if (kint8z.eq.-1) yd8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] if (kint8z.gt.0) yd8z = yd8z*dvol if (kint8z.lt.0) yd8z = yd8z*darea else C############################################################################## C Now enter FORTRAN expressions to define the PDE coefficients, which # C may be functions of # C # C X,Y,Z,U,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz # C V,Vx,Vy,Vz,Vxx,Vyy,Vzz,Vxy,Vxz,Vyz # C W,Wx,Wy,Wz,Wxx,Wyy,Wzz,Wxy,Wxz,Wyz # C # C and, in some cases, of the parameter T. # C # C Recall that the PDEs have the form # C # C F1 = 0 # C F2 = 0 # C F3 = 0 # C # C The parameters P1,P2,P3 and derivatives with respect to these may also # C be referenced (U1 = dU/dP1, etc): # C U1,U2,U3,U11,U22,U33,U12,U13,U23 # C V1,V2,V3,V11,V22,V33,V12,V13,V23 # C W1,W2,W3,W11,W22,W33,W12,W13,W23 # C############################################################################## Rmu = 1. rho = 0.1 alpha = 2.D3 f1 = z f2 = 0 f3 = 0 if (j8z.eq.0) then yd8z = 0.0 C F1 DEFINED if (i8z.eq. 1) yd8z = & Rmu*(Uxx+Uyy+Uzz) -alpha*(Uxx+Vyx+Wzx)-Rho*(U*Ux+V*Uy+W*Uz)+f1 C F2 DEFINED if (i8z.eq. 2) yd8z = & Rmu*(Vxx+Vyy+Vzz) -alpha*(Uxy+Vyy+Wzy)-Rho*(U*Vx+V*Vy+W*Vz)+f2 C F3 DEFINED if (i8z.eq. 3) yd8z = & Rmu*(Wxx+Wyy+Wzz) -alpha*(Uxz+Vyz+Wzz)-Rho*(U*Wx+V*Wy+W*Wz)+f3 else endif endif return end function u8z(i8z,p1,p2,p3,t0) implicit double precision (a-h,o-z) common/parm8z/ pi call dtdpcd(p1,p2,p3) call dtdpcb(p1,p2,p3,zr18z,zr28z,zr38z,x,y,z,d18z,d28z,d38z,1) u8z = 0.0 C############################################################################## C Now the initial values for Newton's method must be defined using # C FORTRAN expressions. They may be functions of X,Y and Z (and the # C parameters P1,P2,P3). # C # C It is important to provide initial values which are at least of the # C correct order of magnitude. # C############################################################################## C U0 DEFINED C if (i8z.eq. 1) u8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] C V0 DEFINED C if (i8z.eq. 2) u8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] C W0 DEFINED C if (i8z.eq. 3) u8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] return end subroutine gb8z(gd8z,ifac8z,i8z,j8z,p1,p2,p3,t,uu8z) implicit double precision (a-h,o-z) parameter (neqnmx= 99) dimension uu8z(10,neqnmx) C un8z(1,I),un8z(2,I),... hold the (rarely used) values C of UI,UI1,... from the previous iteration or time step common /dtdp5x/ un8z(10,neqnmx) common /dtdp18/norm1,norm2,norm3 double precision none,norm1,norm2,norm3,normx,normy,normz common/parm8z/ pi none = dtdplx(2) U = uu8z(1, 1) U1 = uu8z(2, 1) U2 = uu8z(3, 1) U3 = uu8z(4, 1) V = uu8z(1, 2) V1 = uu8z(2, 2) V2 = uu8z(3, 2) V3 = uu8z(4, 2) W = uu8z(1, 3) W1 = uu8z(2, 3) W2 = uu8z(3, 3) W3 = uu8z(4, 3) call dtdpcd(p1,p2,p3) call dtdpcb(p1,p2,p3,norm1,norm2,norm3,x,y,z,normx,normy,normz,3) call dtdpcb( & p1,p2,p3,U1,U2,U3,x,y,z,Ux,Uy,Uz,2) Unorm = Ux*normx + Uy*normy + Uz*normz call dtdpcb( & p1,p2,p3,V1,V2,V3,x,y,z,Vx,Vy,Vz,2) Vnorm = Vx*normx + Vy*normy + Vz*normz call dtdpcb( & p1,p2,p3,W1,W2,W3,x,y,z,Wx,Wy,Wz,2) Wnorm = Wx*normx + Wy*normy + Wz*normz if (j8z.eq.0) gd8z = 0.0 C############################################################################## C Enter FORTRAN expressions to define the boundary condition functions, # C which may be functions of # C # C X,Y,Z,U,Ux,Uy,Uz, # C V,Vx,Vy,Vz, # C W,Wx,Wy,Wz and (if applicable) T # C # C Recall that the boundary conditions have the form # C # C G1 = 0 # C G2 = 0 # C G3 = 0 # C # C Enter NONE to indicate "no" boundary condition. # C # C The parameters P1,P2,P3 and derivatives with respect to these may also # C be referenced (U1 = dU/dP1, etc): # C U1,U2,U3 # C V1,V2,V3 # C W1,W2,W3 # C The components (NORMx,NORMy,NORMz) of the unit outward normal vector # C may also be referenced, as well as the normal derivatives Unorm, # C Vnorm,Wnorm. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + If "no" boundary condition is specified, the corresponding PDE is +# C + enforced at points just inside the boundary (exactly on the +# C + boundary, if EPS8Z is set to 0 in the main program). +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## if (ifac8z.eq. 1) then C############################################################################## C # C First define the boundary conditions on the face P1 = P1GRID(1). # C############################################################################## if (j8z.eq.0) then C G1 DEFINED if (i8z.eq. 1) gd8z = & U C G2 DEFINED if (i8z.eq. 2) gd8z = & V C G3 DEFINED if (i8z.eq. 3) gd8z = & W else endif endif if (ifac8z.eq. 2) then C############################################################################## C # C Now define the boundary conditions on the face P1 = P1GRID(NP1GRID). # C############################################################################## if (j8z.eq.0) then C G1 DEFINED if (i8z.eq. 1) gd8z = & U C G2 DEFINED if (i8z.eq. 2) gd8z = & V C G3 DEFINED if (i8z.eq. 3) gd8z = & W else endif endif if (ifac8z.eq. 3) then C############################################################################## C # C Now define the boundary conditions on the face P2 = P2GRID(1). # C############################################################################## if (j8z.eq.0) then C PERIODIC BOUNDARY CONDITIONS SET (SEE IPERDC) C G1 DEFINED C if (i8z.eq. 1) gd8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] C G2 DEFINED C if (i8z.eq. 2) gd8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] C G3 DEFINED C if (i8z.eq. 3) gd8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] else endif endif if (ifac8z.eq. 4) then C############################################################################## C # C Now define the boundary conditions on the face P2 = P2GRID(NP2GRID). # C############################################################################## if (j8z.eq.0) then C PERIODIC BOUNDARY CONDITIONS SET (SEE IPERDC) C G1 DEFINED C if (i8z.eq. 1) gd8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] C G2 DEFINED C if (i8z.eq. 2) gd8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] C G3 DEFINED C if (i8z.eq. 3) gd8z = C & [DEFAULT SELECTED, DEFINITION COMMENTED OUT] else endif endif if (ifac8z.eq. 5) then C############################################################################## C # C Now define the boundary conditions on the face P3 = P3GRID(1). # C############################################################################## if (j8z.eq.0) then C G1 DEFINED if (i8z.eq. 1) gd8z = & U C G2 DEFINED if (i8z.eq. 2) gd8z = & V C G3 DEFINED if (i8z.eq. 3) gd8z = & W else endif endif if (ifac8z.eq. 6) then C############################################################################## C # C Now define the boundary conditions on the face P3 = P3GRID(NP3GRID). # C############################################################################## if (j8z.eq.0) then G3 = U*NORMx+V*NORMy+W*NORMz if (abs(NORMx).ge.0.5) THEN G1 = NORMy*Unorm - NORMx*Vnorm G2 = NORMz*Unorm - NORMx*Wnorm else if (abs(NORMy).ge.0.5) THEN G1 = NORMy*Unorm - NORMx*Vnorm G2 = NORMz*Vnorm - NORMy*Wnorm else G1 = NORMz*Vnorm - NORMy*Wnorm G2 = NORMz*Unorm - NORMx*Wnorm ENDIF C G1 DEFINED if (i8z.eq. 1) gd8z = & G1 C G2 DEFINED if (i8z.eq. 2) gd8z = & G2 C G3 DEFINED if (i8z.eq. 3) gd8z = & G3 else endif endif return end subroutine pmod8z(p1,p2,p3,t,uu8z,uprint,uxprint,uyprint,uzprint) implicit double precision (a-h,o-z) dimension uu8z(10,*),uprint(*),uxprint(*),uyprint(*),uzprint(*) common/dtdp14/sint(20),bint(20),slim8z(20),blim8z(20) common/parm8z/ pi U = uu8z(1, 1) U1 = uu8z(2, 1) U2 = uu8z(3, 1) U3 = uu8z(4, 1) U11= uu8z(5, 1) U22= uu8z(6, 1) U33= uu8z(7, 1) U12= uu8z(8, 1) U21= uu8z(8, 1) U13= uu8z(9, 1) U31= uu8z(9, 1) U23= uu8z(10, 1) U32= uu8z(10, 1) V = uu8z(1, 2) V1 = uu8z(2, 2) V2 = uu8z(3, 2) V3 = uu8z(4, 2) V11= uu8z(5, 2) V22= uu8z(6, 2) V33= uu8z(7, 2) V12= uu8z(8, 2) V21= uu8z(8, 2) V13= uu8z(9, 2) V31= uu8z(9, 2) V23= uu8z(10, 2) V32= uu8z(10, 2) W = uu8z(1, 3) W1 = uu8z(2, 3) W2 = uu8z(3, 3) W3 = uu8z(4, 3) W11= uu8z(5, 3) W22= uu8z(6, 3) W33= uu8z(7, 3) W12= uu8z(8, 3) W21= uu8z(8, 3) W13= uu8z(9, 3) W31= uu8z(9, 3) W23= uu8z(10, 3) W32= uu8z(10, 3) call dtdpcd(p1,p2,p3) call dtdpcc(p1,p2,p3, & U1,U2,U3,U11,U22,U33,U12,U13,U23, & x,y,z,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz, & Uyx,Uzx,Uzy,dvol8z,dare8z) uxprint( 1) = Ux uyprint( 1) = Uy uzprint( 1) = Uz call dtdpcc(p1,p2,p3, & V1,V2,V3,V11,V22,V33,V12,V13,V23, & x,y,z,Vx,Vy,Vz,Vxx,Vyy,Vzz,Vxy,Vxz,Vyz, & Vyx,Vzx,Vzy,dvol8z,dare8z) uxprint( 2) = Vx uyprint( 2) = Vy uzprint( 2) = Vz call dtdpcc(p1,p2,p3, & W1,W2,W3,W11,W22,W33,W12,W13,W23, & x,y,z,Wx,Wy,Wz,Wxx,Wyy,Wzz,Wxy,Wxz,Wyz, & Wyx,Wzx,Wzy,dvol8z,dare8z) uxprint( 3) = Wx uyprint( 3) = Wy uzprint( 3) = Wz C############################################################################## C If you don't want to read the FINE PRINT, default all of the following # C variables. # C # C +++++++++++++++ THE "FINE PRINT" (CAN USUALLY BE IGNORED) ++++++++++++++# C + Normally, PDE2D saves the values of U,Ux,Uy,Uz,V,Vx, +# C + Vy,Vz,W,Wx,Wy,Wz at the output points. If different +# C + variables are to be saved (for later printing or plotting) the +# C + following functions can be used to re-define the output variables: +# C + define UPRINT(1) to replace U +# C + UXPRINT(1) Ux +# C + UYPRINT(1) Uy +# C + UZPRINT(1) Uz +# C + UPRINT(2) V +# C + UXPRINT(2) Vx +# C + UYPRINT(2) Vy +# C + UZPRINT(2) Vz +# C + UPRINT(3) W +# C + UXPRINT(3) Wx +# C + UYPRINT(3) Wy +# C + UZPRINT(3) Wz +# C + Each function may be a function of +# C + +# C + X,Y,Z,U,Ux,Uy,Uz,Uxx,Uyy,Uzz,Uxy,Uxz,Uyz +# C + V,Vx,Vy,Vz,Vxx,Vyy,Vzz,Vxy,Vxz,Vyz +# C + W,Wx,Wy,Wz,Wxx,Wyy,Wzz,Wxy,Wxz,Wyz +# C + and (if applicable) T +# C + +# C + Each may also be a function of the integral estimates SINT(1),..., +# C + BINT(1),... +# C + +# C + The parameters P1,P2,P3 and derivatives with respect to these may +# C + also be referenced (U1 = dU/dP1, etc): +# C + U1,U2,U3,U11,U22,U33,U12,U13,U23 +# C + V1,V2,V3,V11,V22,V33,V12,V13,V23 +# C + W1,W2,W3,W11,W22,W33,W12,W13,W23 +# C + +# C + The default for each variable is no change, for example, UPRINT(1) +# C + defaults to U. Enter FORTRAN expressions for each of the +# C + following functions (or default). +# C ++++++++++++++++++++++++++ END OF "FINE PRINT" +++++++++++++++++++++++++# C############################################################################## C DEFINE UPRINT(*),UXPRINT(*),UYPRINT(*),UZPRINT(*) HERE: alpha = 2.D3 UPRINT(1) = cos(p1)*U + sin(p1)*V UPRINT(2) =-sin(p1)*U + cos(p1)*V UXPRINT(1) = -alpha*(Ux+Vy+Wz) return end function axis8z(i8z,p1,p2,p3,ical8z) implicit double precision (a-h,o-z) common/parm8z/ pi call dtdpcd(p1,p2,p3) call dtdpcb(p1,p2,p3,zr18z,zr28z,zr38z,x,y,z,d18z,d28z,d38z,1) axis8z = 0.0 if (ical8z.eq. 1) then C############################################################################## C Define the axes A1 and A2 as functions of P2 and P3. A1 and A2 may # C also reference the constant P1 and the Cartesian coordinates X,Y,Z. # C############################################################################## C A1 DEFINED if (i8z.eq. 1) axis8z = & sqrt(x**2+y**2) C A2 DEFINED if (i8z.eq. 2) axis8z = & z endif return end C dummy routines subroutine xy8z(i8z,iarc8z,s,x,y,s0,sf) implicit double precision (a-h,o-z) return end subroutine dis8z(x,y,ktri,triden,shape) implicit double precision (a-h,o-z) return end function fb8z(i8z,iarc8z,ktri,s,x,y,t) implicit double precision (a-h,o-z) fb8z = 0 return end subroutine postpr(tout,nsave,p1out,p2out,p3out,np1,np2,np3,uout,ne &qn,p1grid,p2grid,p3grid,np1grid,np2grid,np3grid) implicit double precision (a-h,o-z) dimension p1out(0:np1,0:np2,0:np3),p2out(0:np1,0:np2,0:np3) dimension p3out(0:np1,0:np2,0:np3),tout(0:nsave) dimension uout(0:np1,0:np2,0:np3,4,neqn,0:nsave) dimension p1grid(np1grid),p2grid(np2grid),p3grid(np3grid) common/parm8z/ pi common /dtdp27/ itask,npes,icomm common /dtdp46/ eps8z,cgtl8z,npmx8z,itype,near8z data lun,lud/0,47/ if (itask.gt.0) return C UOUT(I,J,K,IDER,IEQ,L) = U_IEQ, if IDER=1 C Ux_IEQ, if IDER=2 C Uy_IEQ, if IDER=3 C Uz_IEQ, if IDER=4 C (possibly as modified by UPRINT,..) C at the point (P1OUT(I,J,K) , P2OUT(I,J,K) , P3OUT(I,J,K)) C at time/iteration TOUT(L). C ******* ADD POSTPROCESSING CODE HERE: C IN THE EXAMPLE BELOW, MATLAB PLOTFILES pde2d.m, C pde2d.rdm CREATED (REMOVE COMMENTS TO ACTIVATE) if (lun.eq.0) then lun = 46 open (lun,file='pde2d.m') open (lud,file='pde2d.rdm') write (lun,*) 'fid = fopen(''pde2d.rdm'');' endif do 78750 l=0,nsave if (tout(l).ne.dtdplx(2)) nsave0 = l 78750 continue write (lud,78751) nsave0 write (lud,78751) neqn write (lud,78751) np1grid write (lud,78751) np2grid write (lud,78751) np3grid write (lud,78751) np1 write (lud,78751) np2 write (lud,78751) np3 78751 format (i8) do 78754 i=1,np1grid do 78753 j=1,np2grid do 78752 k=1,np3grid p1 = p1grid(i) p2 = p2grid(j) p3 = p3grid(k) call dtdpcd(p1,p2,p3) call dtdpcb(p1,p2,p3,z18z,z28z,z38z,x,y,z,d18z,d28z,d38z,1) write(lud,78764) x,y,z 78752 continue 78753 continue 78754 continue do 78757 i=0,np1 do 78756 j=0,np2 do 78755 k=0,np3 p1 = p1out(i,j,k) p2 = p2out(i,j,k) p3 = p3out(i,j,k) call dtdpcd(p1,p2,p3) call dtdpcb(p1,p2,p3,z18z,z28z,z38z,x,y,z,d18z,d28z,d38z,1) write(lud,78764) p1,p2,p3,x,y,z 78755 continue 78756 continue 78757 continue if (itype.ne.4) then do 78763 l=0,nsave0 write (lud,78764) tout(l) do 78762 ieq=1,neqn do 78761 ider=1,4 do 78760 i=0,np1 do 78759 j=0,np2 do 78758 k=0,np3 write (lud,78764) uout(i,j,k,ider,ieq,l) 78758 continue 78759 continue 78760 continue 78761 continue 78762 continue 78763 continue 78764 format (e16.8) endif C ******* WRITE pde2d.m call mtdp3d(itype,lun) return end