static char help[] = "Solves the constant-coefficient 1D heat equation \n\ with an Implicit Runge-Kutta method using MatKAIJ. \n\ \n\ du d^2 u \n\ -- = a ----- ; 0 <= x <= 1; \n\ dt dx^2 \n\ \n\ with periodic boundary conditions \n\ \n\ 2nd order central discretization in space: \n\ \n\ [ d^2 u ] u_{i+1} - 2u_i + u_{i-1} \n\ [ ----- ] = ------------------------ \n\ [ dx^2 ]i h^2 \n\ \n\ i = grid index; h = x_{i+1}-x_i (Uniform) \n\ 0 <= i < n h = 1.0/n \n\ \n\ Thus, \n\ \n\ du \n\ -- = Ju; J = (a/h^2) tridiagonal(1,-2,1)_n \n\ dt \n\ \n\ This example is a TS version of the KSP ex74.c tutorial. \n"; #include typedef enum { PHYSICS_DIFFUSION, PHYSICS_ADVECTION } PhysicsType; const char *const PhysicsTypes[] = {"DIFFUSION","ADVECTION","PhysicsType","PHYSICS_",NULL}; typedef struct Context { PetscReal a; /* diffusion coefficient */ PetscReal xmin,xmax; /* domain bounds */ PetscInt imax; /* number of grid points */ PhysicsType physics_type; } UserContext; static PetscErrorCode ExactSolution(Vec,void*,PetscReal); static PetscErrorCode RHSJacobian(TS,PetscReal,Vec,Mat,Mat,void*); int main(int argc, char **argv) { TS ts; Mat A; Vec u,uex; UserContext ctxt; PetscReal err,ftime; PetscErrorCode ierr; PetscCall(PetscInitialize(&argc,&argv,(char*)0,help)); /* default value */ ctxt.a = 0.1; ctxt.xmin = 0.0; ctxt.xmax = 1.0; ctxt.imax = 40; ctxt.physics_type = PHYSICS_DIFFUSION; ierr = PetscOptionsBegin(PETSC_COMM_WORLD,NULL,"IRK options","");PetscCall(ierr); PetscCall(PetscOptionsReal("-a","diffusion coefficient","<1.0>",ctxt.a,&ctxt.a,NULL)); PetscCall(PetscOptionsInt ("-imax","grid size","<20>",ctxt.imax,&ctxt.imax,NULL)); PetscCall(PetscOptionsReal("-xmin","xmin","<0.0>",ctxt.xmin,&ctxt.xmin,NULL)); PetscCall(PetscOptionsReal("-xmax","xmax","<1.0>",ctxt.xmax,&ctxt.xmax,NULL)); PetscCall(PetscOptionsEnum("-physics_type","Type of process to discretize","",PhysicsTypes,(PetscEnum)ctxt.physics_type,(PetscEnum*)&ctxt.physics_type,NULL)); ierr = PetscOptionsEnd();PetscCall(ierr); /* allocate and initialize solution vector and exact solution */ PetscCall(VecCreate(PETSC_COMM_WORLD,&u)); PetscCall(VecSetSizes(u,PETSC_DECIDE,ctxt.imax)); PetscCall(VecSetFromOptions(u)); PetscCall(VecDuplicate(u,&uex)); /* initial solution */ PetscCall(ExactSolution(u,&ctxt,0.0)); PetscCall(MatCreate(PETSC_COMM_WORLD,&A)); PetscCall(MatSetType(A,MATAIJ)); PetscCall(MatSetSizes(A,PETSC_DECIDE,PETSC_DECIDE,ctxt.imax,ctxt.imax)); PetscCall(MatSetUp(A)); /* Create and set options for TS */ PetscCall(TSCreate(PETSC_COMM_WORLD,&ts)); PetscCall(TSSetProblemType(ts,TS_LINEAR)); PetscCall(TSSetTimeStep(ts,0.125)); PetscCall(TSSetSolution(ts,u)); PetscCall(TSSetMaxSteps(ts,10)); PetscCall(TSSetMaxTime(ts,1.0)); PetscCall(TSSetExactFinalTime(ts,TS_EXACTFINALTIME_STEPOVER)); PetscCall(TSSetRHSFunction(ts,NULL,TSComputeRHSFunctionLinear,&ctxt)); PetscCall(RHSJacobian(ts,0,u,A,A,&ctxt)); PetscCall(TSSetRHSJacobian(ts,A,A,TSComputeRHSJacobianConstant,&ctxt)); PetscCall(TSSetFromOptions(ts)); PetscCall(TSSolve(ts,u)); PetscCall(TSGetSolveTime(ts,&ftime)); /* exact solution */ PetscCall(ExactSolution(uex,&ctxt,ftime)); /* Calculate error in final solution */ PetscCall(VecAYPX(uex,-1.0,u)); PetscCall(VecNorm(uex,NORM_2,&err)); err = PetscSqrtReal(err*err/((PetscReal)ctxt.imax)); PetscCall(PetscPrintf(PETSC_COMM_WORLD,"L2 norm of the numerical error = %g (time=%g)\n",(double)err,(double)ftime)); /* Free up memory */ PetscCall(TSDestroy(&ts)); PetscCall(MatDestroy(&A)); PetscCall(VecDestroy(&uex)); PetscCall(VecDestroy(&u)); PetscCall(PetscFinalize()); return 0; } PetscErrorCode ExactSolution(Vec u,void *c,PetscReal t) { UserContext *ctxt = (UserContext*) c; PetscInt i,is,ie; PetscScalar *uarr; PetscReal x,dx,a=ctxt->a,pi=PETSC_PI; PetscFunctionBegin; dx = (ctxt->xmax - ctxt->xmin)/((PetscReal) ctxt->imax); PetscCall(VecGetOwnershipRange(u,&is,&ie)); PetscCall(VecGetArray(u,&uarr)); for (i=is; iphysics_type) { case PHYSICS_DIFFUSION: uarr[i-is] = PetscExpScalar(-4.0*pi*pi*a*t)*PetscSinScalar(2*pi*x); break; case PHYSICS_ADVECTION: uarr[i-is] = PetscSinScalar(2*pi*(x - a*t)); break; default: SETERRQ(PETSC_COMM_SELF,PETSC_ERR_SUP,"No support for physics type %s",PhysicsTypes[ctxt->physics_type]); } } PetscCall(VecRestoreArray(u,&uarr)); PetscFunctionReturn(0); } static PetscErrorCode RHSJacobian(TS ts,PetscReal t,Vec U,Mat J,Mat Jpre,void *ctx) { UserContext *user = (UserContext*) ctx; PetscInt matis,matie,i; PetscReal dx,dx2; PetscFunctionBegin; dx = (user->xmax - user->xmin)/((PetscReal)user->imax); dx2 = dx*dx; PetscCall(MatGetOwnershipRange(J,&matis,&matie)); for (i=matis; iphysics_type) { case PHYSICS_DIFFUSION: values[0] = user->a*1.0/dx2; values[1] = -user->a*2.0/dx2; values[2] = user->a*1.0/dx2; break; case PHYSICS_ADVECTION: values[0] = user->a*.5/dx; values[1] = 0.; values[2] = -user->a*.5/dx; break; default: SETERRQ(PETSC_COMM_SELF,PETSC_ERR_SUP,"No support for physics type %s",PhysicsTypes[user->physics_type]); } /* periodic boundaries */ if (i == 0) { col[0] = user->imax-1; col[1] = i; col[2] = i+1; } else if (i == user->imax-1) { col[0] = i-1; col[1] = i; col[2] = 0; } else { col[0] = i-1; col[1] = i; col[2] = i+1; } PetscCall(MatSetValues(J,1,&i,3,col,values,INSERT_VALUES)); } PetscCall(MatAssemblyBegin(J,MAT_FINAL_ASSEMBLY)); PetscCall(MatAssemblyEnd(J,MAT_FINAL_ASSEMBLY)); PetscFunctionReturn(0); } /*TEST test: requires: double suffix: 1 nsize: {{1 2}} args: -ts_max_steps 5 -ts_monitor -ksp_monitor_short -pc_type pbjacobi -ksp_atol 1e-6 -ts_type irk -ts_irk_nstages 2 test: requires: double suffix: 2 args: -ts_max_steps 5 -ts_monitor -ksp_monitor_short -pc_type pbjacobi -ksp_atol 1e-6 -ts_type irk -ts_irk_nstages 3 testset: requires: hpddm args: -ts_max_steps 5 -ts_monitor -ksp_monitor_short -pc_type pbjacobi -ksp_atol 1e-4 -ts_type irk -ts_irk_nstages 3 -ksp_view_final_residual -ksp_hpddm_type gcrodr -ksp_type hpddm -ksp_hpddm_precision {{single double}shared output} test: suffix: 3 requires: double test: suffix: 3_single requires: single TEST*/