/* Note: -hratio is the ratio between mesh size of coarse grids and fine grids */ static const char help[] = "1D periodic Finite Volume solver in slope-limiter form with semidiscrete time stepping.\n" " advect - Constant coefficient scalar advection\n" " u_t + (a*u)_x = 0\n" " shallow - 1D Shallow water equations (Saint Venant System)\n" " h_t + (q)_x = 0 \n" " q_t + (\frac{q^2}{h} + g/2*h^2)_x = 0 \n" " where, h(x,t) denotes the height of the water and q(x,t) the momentum.\n" " for this toy problem, we choose different meshsizes for different sub-domains (slow-fast-slow), say\n" " hxs = hratio*hxf \n" " where hxs and hxf are the grid spacings for coarse and fine grids respectively.\n" " exact - Exact Riemann solver which usually needs to perform a Newton iteration to connect\n" " the states across shocks and rarefactions\n" " simulation - use reference solution which is generated by smaller time step size to be true solution,\n" " also the reference solution should be generated by user and stored in a binary file.\n" " characteristic - Limit the characteristic variables, this is usually preferred (default)\n" " bc_type - Boundary condition for the problem, options are: periodic, outflow, inflow " "Several problem descriptions (initial data, physics specific features, boundary data) can be chosen with -initial N\n\n" "The problem size should be set with -da_grid_x M\n\n"; /* Example: ./ex4 -da_grid_x 40 -initial 1 -hratio 1 -limit mc -ts_dt 0.01 -ts_max_time 7.0 -ts_type mprk -ts_mprk_type 2a22 -ts_monitor_draw_solution -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 0 ./ex4 -da_grid_x 40 -initial 2 -hratio 1 -limit mc -ts_dt 0.01 -ts_max_time 2.5 -ts_type mprk -ts_mprk_type 2a22 -ts_monitor_draw_solution -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 0 ./ex4 -da_grid_x 40 -initial 3 -hratio 1 -limit mc -ts_dt 0.01 -ts_max_time 4.0 -ts_type mprk -ts_mprk_type 2a22 -ts_monitor_draw_solution -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 0 ./ex4 -da_grid_x 40 -initial 4 -hratio 1 -limit koren3 -ts_dt 0.01 -ts_max_time 4.0 -ts_type mprk -ts_mprk_type 2a22 -ts_monitor_draw_solution -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 0 ./ex4 -da_grid_x 40 -initial 5 -hratio 1 -limit mc -ts_dt 0.01 -ts_max_time 5.0 -ts_type mprk -ts_mprk_type 2a22 -ts_monitor_draw_solution -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 0 Contributed by: Aidan Hamilton */ #include #include #include #include #include "finitevolume1d.h" #include static inline PetscReal RangeMod(PetscReal a, PetscReal xmin, PetscReal xmax) { PetscReal range = xmax - xmin; return xmin + PetscFmodReal(range + PetscFmodReal(a, range), range); } static inline PetscReal MaxAbs(PetscReal a, PetscReal b) { return (PetscAbs(a) > PetscAbs(b)) ? a : b; } /* --------------------------------- Advection ----------------------------------- */ typedef struct { PetscReal a; /* advective velocity */ } AdvectCtx; static PetscErrorCode PhysicsRiemann_Advect(void *vctx, PetscInt m, const PetscScalar *uL, const PetscScalar *uR, PetscScalar *flux, PetscReal *maxspeed) { AdvectCtx *ctx = (AdvectCtx *)vctx; PetscReal speed; PetscFunctionBeginUser; speed = ctx->a; flux[0] = PetscMax(0, speed) * uL[0] + PetscMin(0, speed) * uR[0]; *maxspeed = speed; PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsCharacteristic_Advect(void *vctx, PetscInt m, const PetscScalar *u, PetscScalar *X, PetscScalar *Xi, PetscReal *speeds) { AdvectCtx *ctx = (AdvectCtx *)vctx; PetscFunctionBeginUser; X[0] = 1.; Xi[0] = 1.; speeds[0] = ctx->a; PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsSample_Advect(void *vctx, PetscInt initial, FVBCType bctype, PetscReal xmin, PetscReal xmax, PetscReal t, PetscReal x, PetscReal *u) { AdvectCtx *ctx = (AdvectCtx *)vctx; PetscReal a = ctx->a, x0; PetscFunctionBeginUser; switch (bctype) { case FVBC_OUTFLOW: x0 = x - a * t; break; case FVBC_PERIODIC: x0 = RangeMod(x - a * t, xmin, xmax); break; default: SETERRQ(PETSC_COMM_SELF, PETSC_ERR_ARG_UNKNOWN_TYPE, "unknown BCType"); } switch (initial) { case 0: u[0] = (x0 < 0) ? 1 : -1; break; case 1: u[0] = (x0 < 0) ? -1 : 1; break; case 2: u[0] = (0 < x0 && x0 < 1) ? 1 : 0; break; case 3: u[0] = PetscSinReal(2 * PETSC_PI * x0); break; case 4: u[0] = PetscAbs(x0); break; case 5: u[0] = (x0 < 0 || x0 > 0.5) ? 0 : PetscSqr(PetscSinReal(2 * PETSC_PI * x0)); break; case 6: u[0] = (x0 < 0) ? 0 : ((x0 < 1) ? x0 : ((x0 < 2) ? 2 - x0 : 0)); break; case 7: u[0] = PetscPowReal(PetscSinReal(PETSC_PI * x0), 10.0); break; default: SETERRQ(PETSC_COMM_SELF, PETSC_ERR_ARG_UNKNOWN_TYPE, "unknown initial condition"); } PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsCreate_Advect(FVCtx *ctx) { AdvectCtx *user; PetscFunctionBeginUser; PetscCall(PetscNew(&user)); ctx->physics2.sample2 = PhysicsSample_Advect; ctx->physics2.riemann2 = PhysicsRiemann_Advect; ctx->physics2.characteristic2 = PhysicsCharacteristic_Advect; ctx->physics2.destroy = PhysicsDestroy_SimpleFree; ctx->physics2.user = user; ctx->physics2.dof = 1; PetscCall(PetscStrallocpy("u", &ctx->physics2.fieldname[0])); user->a = 1; PetscOptionsBegin(ctx->comm, ctx->prefix, "Options for advection", ""); PetscCall(PetscOptionsReal("-physics_advect_a", "Speed", "", user->a, &user->a, NULL)); PetscOptionsEnd(); PetscFunctionReturn(PETSC_SUCCESS); } /* --------------------------------- Shallow Water ----------------------------------- */ typedef struct { PetscReal gravity; } ShallowCtx; static inline void ShallowFlux(ShallowCtx *phys, const PetscScalar *u, PetscScalar *f) { f[0] = u[1]; f[1] = PetscSqr(u[1]) / u[0] + 0.5 * phys->gravity * PetscSqr(u[0]); } static PetscErrorCode PhysicsRiemann_Shallow_Exact(void *vctx, PetscInt m, const PetscScalar *uL, const PetscScalar *uR, PetscScalar *flux, PetscReal *maxspeed) { ShallowCtx *phys = (ShallowCtx *)vctx; PetscScalar g = phys->gravity, ustar[2], cL, cR, c, cstar; struct { PetscScalar h, u; } L = {uL[0], uL[1] / uL[0]}, R = {uR[0], uR[1] / uR[0]}, star; PetscInt i; PetscFunctionBeginUser; PetscCheck(L.h > 0 && R.h > 0, PETSC_COMM_SELF, PETSC_ERR_ARG_OUTOFRANGE, "Reconstructed thickness is negative"); cL = PetscSqrtScalar(g * L.h); cR = PetscSqrtScalar(g * R.h); c = PetscMax(cL, cR); { /* Solve for star state */ const PetscInt maxits = 50; PetscScalar tmp, res, res0 = 0, h0, h = 0.5 * (L.h + R.h); /* initial guess */ h0 = h; for (i = 0; i < maxits; i++) { PetscScalar fr, fl, dfr, dfl; fl = (L.h < h) ? PetscSqrtScalar(0.5 * g * (h * h - L.h * L.h) * (1 / L.h - 1 / h)) /* shock */ : 2 * PetscSqrtScalar(g * h) - 2 * PetscSqrtScalar(g * L.h); /* rarefaction */ fr = (R.h < h) ? PetscSqrtScalar(0.5 * g * (h * h - R.h * R.h) * (1 / R.h - 1 / h)) /* shock */ : 2 * PetscSqrtScalar(g * h) - 2 * PetscSqrtScalar(g * R.h); /* rarefaction */ res = R.u - L.u + fr + fl; PetscCheck(!PetscIsInfOrNanScalar(res), PETSC_COMM_SELF, PETSC_ERR_FP, "Infinity or Not-a-Number generated in computation"); if (PetscAbsScalar(res) < PETSC_SQRT_MACHINE_EPSILON || (i > 0 && PetscAbsScalar(h - h0) < PETSC_SQRT_MACHINE_EPSILON)) { star.h = h; star.u = L.u - fl; goto converged; } else if (i > 0 && PetscAbsScalar(res) >= PetscAbsScalar(res0)) { /* Line search */ h = 0.8 * h0 + 0.2 * h; continue; } /* Accept the last step and take another */ res0 = res; h0 = h; dfl = (L.h < h) ? 0.5 / fl * 0.5 * g * (-L.h * L.h / (h * h) - 1 + 2 * h / L.h) : PetscSqrtScalar(g / h); dfr = (R.h < h) ? 0.5 / fr * 0.5 * g * (-R.h * R.h / (h * h) - 1 + 2 * h / R.h) : PetscSqrtScalar(g / h); tmp = h - res / (dfr + dfl); if (tmp <= 0) h /= 2; /* Guard against Newton shooting off to a negative thickness */ else h = tmp; PetscCheck((h > 0) && PetscIsNormalScalar(h), PETSC_COMM_SELF, PETSC_ERR_FP, "non-normal iterate h=%g", (double)h); } SETERRQ(PETSC_COMM_SELF, PETSC_ERR_NOT_CONVERGED, "Newton iteration for star.h diverged after %" PetscInt_FMT " iterations", i); } converged: cstar = PetscSqrtScalar(g * star.h); if (L.u - cL < 0 && 0 < star.u - cstar) { /* 1-wave is sonic rarefaction */ PetscScalar ufan[2]; ufan[0] = 1 / g * PetscSqr(L.u / 3 + 2. / 3 * cL); ufan[1] = PetscSqrtScalar(g * ufan[0]) * ufan[0]; ShallowFlux(phys, ufan, flux); } else if (star.u + cstar < 0 && 0 < R.u + cR) { /* 2-wave is sonic rarefaction */ PetscScalar ufan[2]; ufan[0] = 1 / g * PetscSqr(R.u / 3 - 2. / 3 * cR); ufan[1] = -PetscSqrtScalar(g * ufan[0]) * ufan[0]; ShallowFlux(phys, ufan, flux); } else if ((L.h >= star.h && L.u - c >= 0) || (L.h < star.h && (star.h * star.u - L.h * L.u) / (star.h - L.h) > 0)) { /* 1-wave is right-travelling shock (supersonic) */ ShallowFlux(phys, uL, flux); } else if ((star.h <= R.h && R.u + c <= 0) || (star.h > R.h && (R.h * R.u - star.h * star.h) / (R.h - star.h) < 0)) { /* 2-wave is left-travelling shock (supersonic) */ ShallowFlux(phys, uR, flux); } else { ustar[0] = star.h; ustar[1] = star.h * star.u; ShallowFlux(phys, ustar, flux); } *maxspeed = MaxAbs(MaxAbs(star.u - cstar, star.u + cstar), MaxAbs(L.u - cL, R.u + cR)); PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsRiemann_Shallow_Rusanov(void *vctx, PetscInt m, const PetscScalar *uL, const PetscScalar *uR, PetscScalar *flux, PetscReal *maxspeed) { ShallowCtx *phys = (ShallowCtx *)vctx; PetscScalar g = phys->gravity, fL[2], fR[2], s; struct { PetscScalar h, u; } L = {uL[0], uL[1] / uL[0]}, R = {uR[0], uR[1] / uR[0]}; PetscReal tol = 1e-6; PetscFunctionBeginUser; /* Positivity preserving modification*/ if (L.h < tol) L.u = 0.0; if (R.h < tol) R.u = 0.0; /*simple pos preserve limiter*/ if (L.h < 0) L.h = 0; if (R.h < 0) R.h = 0; ShallowFlux(phys, uL, fL); ShallowFlux(phys, uR, fR); s = PetscMax(PetscAbs(L.u) + PetscSqrtScalar(g * L.h), PetscAbs(R.u) + PetscSqrtScalar(g * R.h)); flux[0] = 0.5 * (fL[0] + fR[0]) + 0.5 * s * (L.h - R.h); flux[1] = 0.5 * (fL[1] + fR[1]) + 0.5 * s * (uL[1] - uR[1]); *maxspeed = s; PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsCharacteristic_Conservative(void *vctx, PetscInt m, const PetscScalar *u, PetscScalar *X, PetscScalar *Xi, PetscReal *speeds) { PetscInt i, j; PetscFunctionBeginUser; for (i = 0; i < m; i++) { for (j = 0; j < m; j++) Xi[i * m + j] = X[i * m + j] = (PetscScalar)(i == j); speeds[i] = PETSC_MAX_REAL; /* Indicates invalid */ } PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsCharacteristic_Shallow(void *vctx, PetscInt m, const PetscScalar *u, PetscScalar *X, PetscScalar *Xi, PetscReal *speeds) { ShallowCtx *phys = (ShallowCtx *)vctx; PetscReal c; PetscReal tol = 1e-6; PetscFunctionBeginUser; c = PetscSqrtScalar(u[0] * phys->gravity); if (u[0] < tol) { /*Use conservative variables*/ X[0 * 2 + 0] = 1; X[0 * 2 + 1] = 0; X[1 * 2 + 0] = 0; X[1 * 2 + 1] = 1; } else { speeds[0] = u[1] / u[0] - c; speeds[1] = u[1] / u[0] + c; X[0 * 2 + 0] = 1; X[0 * 2 + 1] = speeds[0]; X[1 * 2 + 0] = 1; X[1 * 2 + 1] = speeds[1]; } PetscCall(PetscArraycpy(Xi, X, 4)); PetscCall(PetscKernel_A_gets_inverse_A_2(Xi, 0, PETSC_FALSE, NULL)); PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsSample_Shallow(void *vctx, PetscInt initial, FVBCType bctype, PetscReal xmin, PetscReal xmax, PetscReal t, PetscReal x, PetscReal *u) { PetscFunctionBeginUser; PetscCheck(t <= 0, PETSC_COMM_SELF, PETSC_ERR_SUP, "Exact solutions not implemented for t > 0"); switch (initial) { case 0: u[0] = (x < 0) ? 2 : 1; /* Standard Dam Break Problem */ u[1] = (x < 0) ? 0 : 0; break; case 1: u[0] = (x < 10) ? 1 : 0.1; /*The Next 5 problems are standard Riemann problem tests */ u[1] = (x < 10) ? 2.5 : 0; break; case 2: u[0] = (x < 25) ? 1 : 1; u[1] = (x < 25) ? -5 : 5; break; case 3: u[0] = (x < 20) ? 1 : 1e-12; u[1] = (x < 20) ? 0 : 0; break; case 4: u[0] = (x < 30) ? 1e-12 : 1; u[1] = (x < 30) ? 0 : 0; break; case 5: u[0] = (x < 25) ? 0.1 : 0.1; u[1] = (x < 25) ? -0.3 : 0.3; break; case 6: u[0] = 1 + 0.5 * PetscSinReal(2 * PETSC_PI * x); u[1] = 1 * u[0]; break; case 7: if (x < -0.1) { u[0] = 1e-9; u[1] = 0.0; } else if (x < 0.1) { u[0] = 1.0; u[1] = 0.0; } else { u[0] = 1e-9; u[1] = 0.0; } break; case 8: if (x < -0.1) { u[0] = 2; u[1] = 0.0; } else if (x < 0.1) { u[0] = 3.0; u[1] = 0.0; } else { u[0] = 2; u[1] = 0.0; } break; default: SETERRQ(PETSC_COMM_SELF, PETSC_ERR_ARG_UNKNOWN_TYPE, "unknown initial condition"); } PetscFunctionReturn(PETSC_SUCCESS); } /* Implements inflow conditions for the given initial conditions. Which conditions are actually enforced depends on on the results of PhysicsSetInflowType_Shallow. */ static PetscErrorCode PhysicsInflow_Shallow(void *vctx, PetscReal t, PetscReal x, PetscReal *u) { FVCtx *ctx = (FVCtx *)vctx; PetscFunctionBeginUser; if (ctx->bctype == FVBC_INFLOW) { switch (ctx->initial) { case 0: case 1: case 2: case 3: case 4: case 5: u[0] = 0; u[1] = 0.0; /* Left boundary conditions */ u[2] = 0; u[3] = 0.0; /* Right boundary conditions */ break; case 6: u[0] = 0; u[1] = 0.0; /* Left boundary conditions */ u[2] = 0; u[3] = 0.0; /* Right boundary conditions */ break; case 7: u[0] = 0; u[1] = 0.0; /* Left boundary conditions */ u[2] = 0; u[3] = 0.0; /* Right boundary conditions */ break; case 8: u[0] = 0; u[1] = 1.0; /* Left boundary conditions */ u[2] = 0; u[3] = -1.0; /* Right boundary conditions */ break; default: SETERRQ(PETSC_COMM_SELF, PETSC_ERR_ARG_UNKNOWN_TYPE, "unknown initial condition"); } } PetscFunctionReturn(PETSC_SUCCESS); } /* Selects which boundary conditions are marked as inflow and which as outflow when FVBC_INFLOW is selected. */ static PetscErrorCode PhysicsSetInflowType_Shallow(FVCtx *ctx) { PetscFunctionBeginUser; switch (ctx->initial) { case 0: case 1: case 2: case 3: case 4: case 5: case 6: case 7: case 8: /* Fix left and right momentum, height is outflow */ ctx->physics2.bcinflowindex[0] = PETSC_FALSE; ctx->physics2.bcinflowindex[1] = PETSC_TRUE; ctx->physics2.bcinflowindex[2] = PETSC_FALSE; ctx->physics2.bcinflowindex[3] = PETSC_TRUE; break; default: SETERRQ(PETSC_COMM_SELF, PETSC_ERR_ARG_UNKNOWN_TYPE, "unknown initial condition"); } PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode PhysicsCreate_Shallow(FVCtx *ctx) { ShallowCtx *user; PetscFunctionList rlist = 0, rclist = 0; char rname[256] = "rusanov", rcname[256] = "characteristic"; PetscFunctionBeginUser; PetscCall(PetscNew(&user)); ctx->physics2.sample2 = PhysicsSample_Shallow; ctx->physics2.inflow = PhysicsInflow_Shallow; ctx->physics2.destroy = PhysicsDestroy_SimpleFree; ctx->physics2.riemann2 = PhysicsRiemann_Shallow_Rusanov; ctx->physics2.characteristic2 = PhysicsCharacteristic_Shallow; ctx->physics2.user = user; ctx->physics2.dof = 2; PetscCall(PetscMalloc1(2 * (ctx->physics2.dof), &ctx->physics2.bcinflowindex)); PetscCall(PhysicsSetInflowType_Shallow(ctx)); PetscCall(PetscStrallocpy("height", &ctx->physics2.fieldname[0])); PetscCall(PetscStrallocpy("momentum", &ctx->physics2.fieldname[1])); user->gravity = 9.81; PetscCall(RiemannListAdd_2WaySplit(&rlist, "exact", PhysicsRiemann_Shallow_Exact)); PetscCall(RiemannListAdd_2WaySplit(&rlist, "rusanov", PhysicsRiemann_Shallow_Rusanov)); PetscCall(ReconstructListAdd_2WaySplit(&rclist, "characteristic", PhysicsCharacteristic_Shallow)); PetscCall(ReconstructListAdd_2WaySplit(&rclist, "conservative", PhysicsCharacteristic_Conservative)); PetscOptionsBegin(ctx->comm, ctx->prefix, "Options for Shallow", ""); PetscCall(PetscOptionsReal("-physics_shallow_gravity", "Gravity", "", user->gravity, &user->gravity, NULL)); PetscCall(PetscOptionsFList("-physics_shallow_riemann", "Riemann solver", "", rlist, rname, rname, sizeof(rname), NULL)); PetscCall(PetscOptionsFList("-physics_shallow_reconstruct", "Reconstruction", "", rclist, rcname, rcname, sizeof(rcname), NULL)); PetscOptionsEnd(); PetscCall(RiemannListFind_2WaySplit(rlist, rname, &ctx->physics2.riemann2)); PetscCall(ReconstructListFind_2WaySplit(rclist, rcname, &ctx->physics2.characteristic2)); PetscCall(PetscFunctionListDestroy(&rlist)); PetscCall(PetscFunctionListDestroy(&rclist)); PetscFunctionReturn(PETSC_SUCCESS); } PetscErrorCode FVSample_2WaySplit(FVCtx *ctx, DM da, PetscReal time, Vec U) { PetscScalar *u, *uj, xj, xi; PetscInt i, j, k, dof, xs, xm, Mx; const PetscInt N = 200; PetscReal hs, hf; PetscFunctionBeginUser; PetscCheck(ctx->physics2.sample2, PETSC_COMM_SELF, PETSC_ERR_SUP, "Physics has not provided a sampling function"); PetscCall(DMDAGetInfo(da, 0, &Mx, 0, 0, 0, 0, 0, &dof, 0, 0, 0, 0, 0)); PetscCall(DMDAGetCorners(da, &xs, 0, 0, &xm, 0, 0)); PetscCall(DMDAVecGetArray(da, U, &u)); PetscCall(PetscMalloc1(dof, &uj)); hs = (ctx->xmax - ctx->xmin) * 3.0 / 8.0 / ctx->sf; hf = (ctx->xmax - ctx->xmin) / 4.0 / (ctx->fs - ctx->sf); for (i = xs; i < xs + xm; i++) { if (i < ctx->sf) { xi = ctx->xmin + 0.5 * hs + i * hs; /* Integrate over cell i using trapezoid rule with N points. */ for (k = 0; k < dof; k++) u[i * dof + k] = 0; for (j = 0; j < N + 1; j++) { xj = xi + hs * (j - N / 2) / (PetscReal)N; PetscCall((*ctx->physics2.sample2)(ctx->physics2.user, ctx->initial, ctx->bctype, ctx->xmin, ctx->xmax, time, xj, uj)); for (k = 0; k < dof; k++) u[i * dof + k] += ((j == 0 || j == N) ? 0.5 : 1.0) * uj[k] / N; } } else if (i < ctx->fs) { xi = ctx->xmin + ctx->sf * hs + 0.5 * hf + (i - ctx->sf) * hf; /* Integrate over cell i using trapezoid rule with N points. */ for (k = 0; k < dof; k++) u[i * dof + k] = 0; for (j = 0; j < N + 1; j++) { xj = xi + hf * (j - N / 2) / (PetscReal)N; PetscCall((*ctx->physics2.sample2)(ctx->physics2.user, ctx->initial, ctx->bctype, ctx->xmin, ctx->xmax, time, xj, uj)); for (k = 0; k < dof; k++) u[i * dof + k] += ((j == 0 || j == N) ? 0.5 : 1.0) * uj[k] / N; } } else { xi = ctx->xmin + ctx->sf * hs + (ctx->fs - ctx->sf) * hf + 0.5 * hs + (i - ctx->fs) * hs; /* Integrate over cell i using trapezoid rule with N points. */ for (k = 0; k < dof; k++) u[i * dof + k] = 0; for (j = 0; j < N + 1; j++) { xj = xi + hs * (j - N / 2) / (PetscReal)N; PetscCall((*ctx->physics2.sample2)(ctx->physics2.user, ctx->initial, ctx->bctype, ctx->xmin, ctx->xmax, time, xj, uj)); for (k = 0; k < dof; k++) u[i * dof + k] += ((j == 0 || j == N) ? 0.5 : 1.0) * uj[k] / N; } } } PetscCall(DMDAVecRestoreArray(da, U, &u)); PetscCall(PetscFree(uj)); PetscFunctionReturn(PETSC_SUCCESS); } static PetscErrorCode SolutionErrorNorms_2WaySplit(FVCtx *ctx, DM da, PetscReal t, Vec X, PetscReal *nrm1) { Vec Y; PetscInt i, Mx; const PetscScalar *ptr_X, *ptr_Y; PetscReal hs, hf; PetscFunctionBeginUser; PetscCall(VecGetSize(X, &Mx)); PetscCall(VecDuplicate(X, &Y)); PetscCall(FVSample_2WaySplit(ctx, da, t, Y)); hs = (ctx->xmax - ctx->xmin) * 3.0 / 8.0 / ctx->sf; hf = (ctx->xmax - ctx->xmin) / 4.0 / (ctx->fs - ctx->sf); PetscCall(VecGetArrayRead(X, &ptr_X)); PetscCall(VecGetArrayRead(Y, &ptr_Y)); for (i = 0; i < Mx; i++) { if (i < ctx->sf || i > ctx->fs - 1) *nrm1 += hs * PetscAbs(ptr_X[i] - ptr_Y[i]); else *nrm1 += hf * PetscAbs(ptr_X[i] - ptr_Y[i]); } PetscCall(VecRestoreArrayRead(X, &ptr_X)); PetscCall(VecRestoreArrayRead(Y, &ptr_Y)); PetscCall(VecDestroy(&Y)); PetscFunctionReturn(PETSC_SUCCESS); } PetscErrorCode FVRHSFunction_2WaySplit(TS ts, PetscReal time, Vec X, Vec F, void *vctx) { FVCtx *ctx = (FVCtx *)vctx; PetscInt i, j, k, Mx, dof, xs, xm, sf = ctx->sf, fs = ctx->fs; PetscReal hxf, hxs, cfl_idt = 0; PetscScalar *x, *f, *slope; Vec Xloc; DM da; PetscFunctionBeginUser; PetscCall(TSGetDM(ts, &da)); PetscCall(DMGetLocalVector(da, &Xloc)); /* Xloc contains ghost points */ PetscCall(DMDAGetInfo(da, 0, &Mx, 0, 0, 0, 0, 0, &dof, 0, 0, 0, 0, 0)); /* Mx is the number of center points */ hxs = (ctx->xmax - ctx->xmin) * 3.0 / 8.0 / ctx->sf; hxf = (ctx->xmax - ctx->xmin) / 4.0 / (ctx->fs - ctx->sf); PetscCall(DMGlobalToLocalBegin(da, X, INSERT_VALUES, Xloc)); /* X is solution vector which does not contain ghost points */ PetscCall(DMGlobalToLocalEnd(da, X, INSERT_VALUES, Xloc)); PetscCall(VecZeroEntries(F)); /* F is the right-hand side function corresponds to center points */ PetscCall(DMDAVecGetArray(da, Xloc, &x)); PetscCall(DMDAVecGetArray(da, F, &f)); PetscCall(DMDAGetArray(da, PETSC_TRUE, &slope)); /* contains ghost points */ PetscCall(DMDAGetCorners(da, &xs, 0, 0, &xm, 0, 0)); if (ctx->bctype == FVBC_OUTFLOW) { for (i = xs - 2; i < 0; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[j]; } for (i = Mx; i < xs + xm + 2; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[(xs + xm - 1) * dof + j]; } } if (ctx->bctype == FVBC_INFLOW) { /* See LeVeque, R. (2002). Finite Volume Methods for Hyperbolic Problems. doi:10.1017/CBO9780511791253 pages 137-138 for the scheme. */ if (xs == 0) { /* Left Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmin, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[j]) { for (i = -2; i < 0; i++) x[i * dof + j] = 2.0 * ctx->ub[j] - x[-(i + 1) * dof + j]; } else { for (i = -2; i < 0; i++) x[i * dof + j] = x[j]; /* Outflow */ } } } if (xs + xm == Mx) { /* Right Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmax, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[dof + j]) { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = 2.0 * ctx->ub[dof + j] - x[(2 * Mx - (i + 1)) * dof + j]; } else { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = x[(Mx - 1) * dof + j]; /* Outflow */ } } } } for (i = xs - 1; i < xs + xm + 1; i++) { struct _LimitInfo info; PetscScalar *cjmpL, *cjmpR; /* Determine the right eigenvectors R, where A = R \Lambda R^{-1} */ PetscCall((*ctx->physics2.characteristic2)(ctx->physics2.user, dof, &x[i * dof], ctx->R, ctx->Rinv, ctx->speeds)); /* Evaluate jumps across interfaces (i-1, i) and (i, i+1), put in characteristic basis */ PetscCall(PetscArrayzero(ctx->cjmpLR, 2 * dof)); cjmpL = &ctx->cjmpLR[0]; cjmpR = &ctx->cjmpLR[dof]; for (j = 0; j < dof; j++) { PetscScalar jmpL, jmpR; jmpL = x[(i + 0) * dof + j] - x[(i - 1) * dof + j]; jmpR = x[(i + 1) * dof + j] - x[(i + 0) * dof + j]; for (k = 0; k < dof; k++) { cjmpL[k] += ctx->Rinv[k + j * dof] * jmpL; cjmpR[k] += ctx->Rinv[k + j * dof] * jmpR; } } /* Apply limiter to the left and right characteristic jumps */ info.m = dof; info.hxs = hxs; info.hxf = hxf; (*ctx->limit2)(&info, cjmpL, cjmpR, ctx->sf, ctx->fs, i, ctx->cslope); for (j = 0; j < dof; j++) { PetscScalar tmp = 0; for (k = 0; k < dof; k++) tmp += ctx->R[j + k * dof] * ctx->cslope[k]; slope[i * dof + j] = tmp; } } for (i = xs; i < xs + xm + 1; i++) { PetscReal maxspeed; PetscScalar *uL, *uR; uL = &ctx->uLR[0]; uR = &ctx->uLR[dof]; if (i < sf) { /* slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(i - 1) * dof + j] -= ctx->flux[j] / hxs; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[i * dof + j] += ctx->flux[j] / hxs; } } else if (i == sf) { /* interface between the slow region and the fast region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxf / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(i - 1) * dof + j] -= ctx->flux[j] / hxs; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[i * dof + j] += ctx->flux[j] / hxf; } } else if (i > sf && i < fs) { /* fast region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxf / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxf / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(i - 1) * dof + j] -= ctx->flux[j] / hxf; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[i * dof + j] += ctx->flux[j] / hxf; } } else if (i == fs) { /* interface between the fast region and the slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxf / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(i - 1) * dof + j] -= ctx->flux[j] / hxf; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[i * dof + j] += ctx->flux[j] / hxs; } } else { /* slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); cfl_idt = PetscMax(cfl_idt, PetscAbsScalar(maxspeed / hxs)); /* Max allowable value of 1/Delta t */ if (i > xs) { for (j = 0; j < dof; j++) f[(i - 1) * dof + j] -= ctx->flux[j] / hxs; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[i * dof + j] += ctx->flux[j] / hxs; } } } PetscCall(DMDAVecRestoreArray(da, Xloc, &x)); PetscCall(DMDAVecRestoreArray(da, F, &f)); PetscCall(DMDARestoreArray(da, PETSC_TRUE, &slope)); PetscCall(DMRestoreLocalVector(da, &Xloc)); PetscCallMPI(MPIU_Allreduce(&cfl_idt, &ctx->cfl_idt, 1, MPIU_SCALAR, MPIU_MAX, PetscObjectComm((PetscObject)da))); if (0) { /* We need to a way to inform the TS of a CFL constraint, this is a debugging fragment */ PetscReal dt, tnow; PetscCall(TSGetTimeStep(ts, &dt)); PetscCall(TSGetTime(ts, &tnow)); if (dt > 0.5 / ctx->cfl_idt) { if (1) { PetscCall(PetscPrintf(ctx->comm, "Stability constraint exceeded at t=%g, dt %g > %g\n", (double)tnow, (double)dt, (double)(0.5 / ctx->cfl_idt))); } else SETERRQ(PETSC_COMM_SELF, PETSC_ERR_PLIB, "Stability constraint exceeded, %g > %g", (double)dt, (double)(ctx->cfl / ctx->cfl_idt)); } } PetscFunctionReturn(PETSC_SUCCESS); } /* --------------------------------- Finite Volume Solver for slow components ----------------------------------- */ PetscErrorCode FVRHSFunctionslow_2WaySplit(TS ts, PetscReal time, Vec X, Vec F, void *vctx) { FVCtx *ctx = (FVCtx *)vctx; PetscInt i, j, k, Mx, dof, xs, xm, islow = 0, sf = ctx->sf, fs = ctx->fs, lsbwidth = ctx->lsbwidth, rsbwidth = ctx->rsbwidth; PetscReal hxs, hxf, cfl_idt = 0; PetscScalar *x, *f, *slope; Vec Xloc; DM da; PetscFunctionBeginUser; PetscCall(TSGetDM(ts, &da)); PetscCall(DMGetLocalVector(da, &Xloc)); PetscCall(DMDAGetInfo(da, 0, &Mx, 0, 0, 0, 0, 0, &dof, 0, 0, 0, 0, 0)); hxs = (ctx->xmax - ctx->xmin) * 3.0 / 8.0 / ctx->sf; hxf = (ctx->xmax - ctx->xmin) / 4.0 / (ctx->fs - ctx->sf); PetscCall(DMGlobalToLocalBegin(da, X, INSERT_VALUES, Xloc)); PetscCall(DMGlobalToLocalEnd(da, X, INSERT_VALUES, Xloc)); PetscCall(VecZeroEntries(F)); PetscCall(DMDAVecGetArray(da, Xloc, &x)); PetscCall(VecGetArray(F, &f)); PetscCall(DMDAGetArray(da, PETSC_TRUE, &slope)); PetscCall(DMDAGetCorners(da, &xs, 0, 0, &xm, 0, 0)); if (ctx->bctype == FVBC_OUTFLOW) { for (i = xs - 2; i < 0; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[j]; } for (i = Mx; i < xs + xm + 2; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[(xs + xm - 1) * dof + j]; } } if (ctx->bctype == FVBC_INFLOW) { /* See LeVeque, R. (2002). Finite Volume Methods for Hyperbolic Problems. doi:10.1017/CBO9780511791253 pages 137-138 for the scheme. */ if (xs == 0) { /* Left Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmin, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[j] == PETSC_TRUE) { for (i = -2; i < 0; i++) x[i * dof + j] = 2.0 * ctx->ub[j] - x[-(i + 1) * dof + j]; } else { for (i = -2; i < 0; i++) x[i * dof + j] = x[j]; /* Outflow */ } } } if (xs + xm == Mx) { /* Right Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmax, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[dof + j] == PETSC_TRUE) { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = 2.0 * ctx->ub[dof + j] - x[(2 * Mx - (i + 1)) * dof + j]; } else { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = x[(Mx - 1) * dof + j]; /* Outflow */ } } } } for (i = xs - 1; i < xs + xm + 1; i++) { struct _LimitInfo info; PetscScalar *cjmpL, *cjmpR; if (i < sf - lsbwidth + 1 || i > fs + rsbwidth - 2) { /* slow components and the first and last fast components */ /* Determine the right eigenvectors R, where A = R \Lambda R^{-1} */ PetscCall((*ctx->physics2.characteristic2)(ctx->physics2.user, dof, &x[i * dof], ctx->R, ctx->Rinv, ctx->speeds)); /* Evaluate jumps across interfaces (i-1, i) and (i, i+1), put in characteristic basis */ PetscCall(PetscArrayzero(ctx->cjmpLR, 2 * dof)); cjmpL = &ctx->cjmpLR[0]; cjmpR = &ctx->cjmpLR[dof]; for (j = 0; j < dof; j++) { PetscScalar jmpL, jmpR; jmpL = x[(i + 0) * dof + j] - x[(i - 1) * dof + j]; jmpR = x[(i + 1) * dof + j] - x[(i + 0) * dof + j]; for (k = 0; k < dof; k++) { cjmpL[k] += ctx->Rinv[k + j * dof] * jmpL; cjmpR[k] += ctx->Rinv[k + j * dof] * jmpR; } } /* Apply limiter to the left and right characteristic jumps */ info.m = dof; info.hxs = hxs; info.hxf = hxf; (*ctx->limit2)(&info, cjmpL, cjmpR, ctx->sf, ctx->fs, i, ctx->cslope); for (j = 0; j < dof; j++) { PetscScalar tmp = 0; for (k = 0; k < dof; k++) tmp += ctx->R[j + k * dof] * ctx->cslope[k]; slope[i * dof + j] = tmp; } } } for (i = xs; i < xs + xm + 1; i++) { PetscReal maxspeed; PetscScalar *uL, *uR; uL = &ctx->uLR[0]; uR = &ctx->uLR[dof]; if (i < sf - lsbwidth) { /* slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); cfl_idt = PetscMax(cfl_idt, PetscAbsScalar(maxspeed / hxs)); /* Max allowable value of 1/Delta t */ if (i > xs) { for (j = 0; j < dof; j++) f[(islow - 1) * dof + j] -= ctx->flux[j] / hxs; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[islow * dof + j] += ctx->flux[j] / hxs; islow++; } } if (i == sf - lsbwidth) { /* interface between the slow region and the fast region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(islow - 1) * dof + j] -= ctx->flux[j] / hxs; } } if (i == fs + rsbwidth) { /* slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i < xs + xm) { for (j = 0; j < dof; j++) f[islow * dof + j] += ctx->flux[j] / hxs; islow++; } } if (i > fs + rsbwidth) { /* slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(islow - 1) * dof + j] -= ctx->flux[j] / hxs; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[islow * dof + j] += ctx->flux[j] / hxs; islow++; } } } PetscCall(DMDAVecRestoreArray(da, Xloc, &x)); PetscCall(VecRestoreArray(F, &f)); PetscCall(DMDARestoreArray(da, PETSC_TRUE, &slope)); PetscCall(DMRestoreLocalVector(da, &Xloc)); PetscCallMPI(MPIU_Allreduce(&cfl_idt, &ctx->cfl_idt, 1, MPIU_SCALAR, MPIU_MAX, PetscObjectComm((PetscObject)da))); PetscFunctionReturn(PETSC_SUCCESS); } PetscErrorCode FVRHSFunctionslowbuffer_2WaySplit(TS ts, PetscReal time, Vec X, Vec F, void *vctx) { FVCtx *ctx = (FVCtx *)vctx; PetscInt i, j, k, Mx, dof, xs, xm, islow = 0, sf = ctx->sf, fs = ctx->fs, lsbwidth = ctx->lsbwidth, rsbwidth = ctx->rsbwidth; PetscReal hxs, hxf; PetscScalar *x, *f, *slope; Vec Xloc; DM da; PetscFunctionBeginUser; PetscCall(TSGetDM(ts, &da)); PetscCall(DMGetLocalVector(da, &Xloc)); PetscCall(DMDAGetInfo(da, 0, &Mx, 0, 0, 0, 0, 0, &dof, 0, 0, 0, 0, 0)); hxs = (ctx->xmax - ctx->xmin) * 3.0 / 8.0 / ctx->sf; hxf = (ctx->xmax - ctx->xmin) / 4.0 / (ctx->fs - ctx->sf); PetscCall(DMGlobalToLocalBegin(da, X, INSERT_VALUES, Xloc)); PetscCall(DMGlobalToLocalEnd(da, X, INSERT_VALUES, Xloc)); PetscCall(VecZeroEntries(F)); PetscCall(DMDAVecGetArray(da, Xloc, &x)); PetscCall(VecGetArray(F, &f)); PetscCall(DMDAGetArray(da, PETSC_TRUE, &slope)); PetscCall(DMDAGetCorners(da, &xs, 0, 0, &xm, 0, 0)); if (ctx->bctype == FVBC_OUTFLOW) { for (i = xs - 2; i < 0; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[j]; } for (i = Mx; i < xs + xm + 2; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[(xs + xm - 1) * dof + j]; } } if (ctx->bctype == FVBC_INFLOW) { /* See LeVeque, R. (2002). Finite Volume Methods for Hyperbolic Problems. doi:10.1017/CBO9780511791253 pages 137-138 for the scheme. */ if (xs == 0) { /* Left Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmin, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[j] == PETSC_TRUE) { for (i = -2; i < 0; i++) x[i * dof + j] = 2.0 * ctx->ub[j] - x[-(i + 1) * dof + j]; } else { for (i = -2; i < 0; i++) x[i * dof + j] = x[j]; /* Outflow */ } } } if (xs + xm == Mx) { /* Right Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmax, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[dof + j] == PETSC_TRUE) { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = 2.0 * ctx->ub[dof + j] - x[(2 * Mx - (i + 1)) * dof + j]; } else { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = x[(Mx - 1) * dof + j]; /* Outflow */ } } } } for (i = xs - 1; i < xs + xm + 1; i++) { struct _LimitInfo info; PetscScalar *cjmpL, *cjmpR; if ((i > sf - lsbwidth - 2 && i < sf + 1) || (i > fs - 2 && i < fs + rsbwidth + 1)) { /* Determine the right eigenvectors R, where A = R \Lambda R^{-1} */ PetscCall((*ctx->physics2.characteristic2)(ctx->physics2.user, dof, &x[i * dof], ctx->R, ctx->Rinv, ctx->speeds)); /* Evaluate jumps across interfaces (i-1, i) and (i, i+1), put in characteristic basis */ PetscCall(PetscArrayzero(ctx->cjmpLR, 2 * dof)); cjmpL = &ctx->cjmpLR[0]; cjmpR = &ctx->cjmpLR[dof]; for (j = 0; j < dof; j++) { PetscScalar jmpL, jmpR; jmpL = x[(i + 0) * dof + j] - x[(i - 1) * dof + j]; jmpR = x[(i + 1) * dof + j] - x[(i + 0) * dof + j]; for (k = 0; k < dof; k++) { cjmpL[k] += ctx->Rinv[k + j * dof] * jmpL; cjmpR[k] += ctx->Rinv[k + j * dof] * jmpR; } } /* Apply limiter to the left and right characteristic jumps */ info.m = dof; info.hxs = hxs; info.hxf = hxf; (*ctx->limit2)(&info, cjmpL, cjmpR, ctx->sf, ctx->fs, i, ctx->cslope); for (j = 0; j < dof; j++) { PetscScalar tmp = 0; for (k = 0; k < dof; k++) tmp += ctx->R[j + k * dof] * ctx->cslope[k]; slope[i * dof + j] = tmp; } } } for (i = xs; i < xs + xm + 1; i++) { PetscReal maxspeed; PetscScalar *uL, *uR; uL = &ctx->uLR[0]; uR = &ctx->uLR[dof]; if (i == sf - lsbwidth) { for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i < xs + xm) { for (j = 0; j < dof; j++) f[islow * dof + j] += ctx->flux[j] / hxs; islow++; } } if (i > sf - lsbwidth && i < sf) { for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(islow - 1) * dof + j] -= ctx->flux[j] / hxs; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[islow * dof + j] += ctx->flux[j] / hxs; islow++; } } if (i == sf) { /* interface between the slow region and the fast region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxf / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(islow - 1) * dof + j] -= ctx->flux[j] / hxs; } } if (i == fs) { /* interface between the fast region and the slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxf / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i < xs + xm) { for (j = 0; j < dof; j++) f[islow * dof + j] += ctx->flux[j] / hxs; islow++; } } if (i > fs && i < fs + rsbwidth) { for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(islow - 1) * dof + j] -= ctx->flux[j] / hxs; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[islow * dof + j] += ctx->flux[j] / hxs; islow++; } } if (i == fs + rsbwidth) { for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(islow - 1) * dof + j] -= ctx->flux[j] / hxs; } } } PetscCall(DMDAVecRestoreArray(da, Xloc, &x)); PetscCall(VecRestoreArray(F, &f)); PetscCall(DMDARestoreArray(da, PETSC_TRUE, &slope)); PetscCall(DMRestoreLocalVector(da, &Xloc)); PetscFunctionReturn(PETSC_SUCCESS); } /* --------------------------------- Finite Volume Solver for fast parts ----------------------------------- */ PetscErrorCode FVRHSFunctionfast_2WaySplit(TS ts, PetscReal time, Vec X, Vec F, void *vctx) { FVCtx *ctx = (FVCtx *)vctx; PetscInt i, j, k, Mx, dof, xs, xm, ifast = 0, sf = ctx->sf, fs = ctx->fs; PetscReal hxs, hxf; PetscScalar *x, *f, *slope; Vec Xloc; DM da; PetscFunctionBeginUser; PetscCall(TSGetDM(ts, &da)); PetscCall(DMGetLocalVector(da, &Xloc)); PetscCall(DMDAGetInfo(da, 0, &Mx, 0, 0, 0, 0, 0, &dof, 0, 0, 0, 0, 0)); hxs = (ctx->xmax - ctx->xmin) * 3.0 / 8.0 / ctx->sf; hxf = (ctx->xmax - ctx->xmin) / 4.0 / (ctx->fs - ctx->sf); PetscCall(DMGlobalToLocalBegin(da, X, INSERT_VALUES, Xloc)); PetscCall(DMGlobalToLocalEnd(da, X, INSERT_VALUES, Xloc)); PetscCall(VecZeroEntries(F)); PetscCall(DMDAVecGetArray(da, Xloc, &x)); PetscCall(VecGetArray(F, &f)); PetscCall(DMDAGetArray(da, PETSC_TRUE, &slope)); PetscCall(DMDAGetCorners(da, &xs, 0, 0, &xm, 0, 0)); if (ctx->bctype == FVBC_OUTFLOW) { for (i = xs - 2; i < 0; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[j]; } for (i = Mx; i < xs + xm + 2; i++) { for (j = 0; j < dof; j++) x[i * dof + j] = x[(xs + xm - 1) * dof + j]; } } if (ctx->bctype == FVBC_INFLOW) { /* See LeVeque, R. (2002). Finite Volume Methods for Hyperbolic Problems. doi:10.1017/CBO9780511791253 pages 137-138 for the scheme. */ if (xs == 0) { /* Left Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmin, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[j] == PETSC_TRUE) { for (i = -2; i < 0; i++) x[i * dof + j] = 2.0 * ctx->ub[j] - x[-(i + 1) * dof + j]; } else { for (i = -2; i < 0; i++) x[i * dof + j] = x[j]; /* Outflow */ } } } if (xs + xm == Mx) { /* Right Boundary */ PetscCall(ctx->physics2.inflow(ctx, time, ctx->xmax, ctx->ub)); for (j = 0; j < dof; j++) { if (ctx->physics2.bcinflowindex[dof + j] == PETSC_TRUE) { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = 2.0 * ctx->ub[dof + j] - x[(2 * Mx - (i + 1)) * dof + j]; } else { for (i = Mx; i < Mx + 2; i++) x[i * dof + j] = x[(Mx - 1) * dof + j]; /* Outflow */ } } } } for (i = xs - 1; i < xs + xm + 1; i++) { struct _LimitInfo info; PetscScalar *cjmpL, *cjmpR; if (i > sf - 2 && i < fs + 1) { PetscCall((*ctx->physics2.characteristic2)(ctx->physics2.user, dof, &x[i * dof], ctx->R, ctx->Rinv, ctx->speeds)); PetscCall(PetscArrayzero(ctx->cjmpLR, 2 * dof)); cjmpL = &ctx->cjmpLR[0]; cjmpR = &ctx->cjmpLR[dof]; for (j = 0; j < dof; j++) { PetscScalar jmpL, jmpR; jmpL = x[(i + 0) * dof + j] - x[(i - 1) * dof + j]; jmpR = x[(i + 1) * dof + j] - x[(i + 0) * dof + j]; for (k = 0; k < dof; k++) { cjmpL[k] += ctx->Rinv[k + j * dof] * jmpL; cjmpR[k] += ctx->Rinv[k + j * dof] * jmpR; } } /* Apply limiter to the left and right characteristic jumps */ info.m = dof; info.hxs = hxs; info.hxf = hxf; (*ctx->limit2)(&info, cjmpL, cjmpR, ctx->sf, ctx->fs, i, ctx->cslope); for (j = 0; j < dof; j++) { PetscScalar tmp = 0; for (k = 0; k < dof; k++) tmp += ctx->R[j + k * dof] * ctx->cslope[k]; slope[i * dof + j] = tmp; } } } for (i = xs; i < xs + xm + 1; i++) { PetscReal maxspeed; PetscScalar *uL, *uR; uL = &ctx->uLR[0]; uR = &ctx->uLR[dof]; if (i == sf) { /* interface between the slow region and the fast region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxs / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxf / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i < xs + xm) { for (j = 0; j < dof; j++) f[ifast * dof + j] += ctx->flux[j] / hxf; ifast++; } } if (i > sf && i < fs) { /* fast region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxf / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxf / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(ifast - 1) * dof + j] -= ctx->flux[j] / hxf; } if (i < xs + xm) { for (j = 0; j < dof; j++) f[ifast * dof + j] += ctx->flux[j] / hxf; ifast++; } } if (i == fs) { /* interface between the fast region and the slow region */ for (j = 0; j < dof; j++) { uL[j] = x[(i - 1) * dof + j] + slope[(i - 1) * dof + j] * hxf / 2; uR[j] = x[(i - 0) * dof + j] - slope[(i - 0) * dof + j] * hxs / 2; } PetscCall((*ctx->physics2.riemann2)(ctx->physics2.user, dof, uL, uR, ctx->flux, &maxspeed)); if (i > xs) { for (j = 0; j < dof; j++) f[(ifast - 1) * dof + j] -= ctx->flux[j] / hxf; } } } PetscCall(DMDAVecRestoreArray(da, Xloc, &x)); PetscCall(VecRestoreArray(F, &f)); PetscCall(DMDARestoreArray(da, PETSC_TRUE, &slope)); PetscCall(DMRestoreLocalVector(da, &Xloc)); PetscFunctionReturn(PETSC_SUCCESS); } int main(int argc, char *argv[]) { char lname[256] = "mc", physname[256] = "advect", final_fname[256] = "solution.m"; PetscFunctionList limiters = 0, physics = 0; MPI_Comm comm; TS ts; DM da; Vec X, X0, R; FVCtx ctx; PetscInt i, k, dof, xs, xm, Mx, draw = 0, count_slow, count_fast, islow = 0, ifast = 0, islowbuffer = 0, *index_slow, *index_fast, *index_slowbuffer; PetscBool view_final = PETSC_FALSE; PetscReal ptime, maxtime; PetscFunctionBeginUser; PetscCall(PetscInitialize(&argc, &argv, 0, help)); comm = PETSC_COMM_WORLD; PetscCall(PetscMemzero(&ctx, sizeof(ctx))); /* Register limiters to be available on the command line */ PetscCall(PetscFunctionListAdd(&limiters, "upwind", Limit2_Upwind)); PetscCall(PetscFunctionListAdd(&limiters, "lax-wendroff", Limit2_LaxWendroff)); PetscCall(PetscFunctionListAdd(&limiters, "beam-warming", Limit2_BeamWarming)); PetscCall(PetscFunctionListAdd(&limiters, "fromm", Limit2_Fromm)); PetscCall(PetscFunctionListAdd(&limiters, "minmod", Limit2_Minmod)); PetscCall(PetscFunctionListAdd(&limiters, "superbee", Limit2_Superbee)); PetscCall(PetscFunctionListAdd(&limiters, "mc", Limit2_MC)); PetscCall(PetscFunctionListAdd(&limiters, "koren3", Limit2_Koren3)); /* Register physical models to be available on the command line */ PetscCall(PetscFunctionListAdd(&physics, "shallow", PhysicsCreate_Shallow)); PetscCall(PetscFunctionListAdd(&physics, "advect", PhysicsCreate_Advect)); ctx.comm = comm; ctx.cfl = 0.9; ctx.bctype = FVBC_PERIODIC; ctx.xmin = -1.0; ctx.xmax = 1.0; ctx.initial = 1; ctx.hratio = 2; maxtime = 10.0; ctx.simulation = PETSC_FALSE; PetscOptionsBegin(comm, NULL, "Finite Volume solver options", ""); PetscCall(PetscOptionsReal("-xmin", "X min", "", ctx.xmin, &ctx.xmin, NULL)); PetscCall(PetscOptionsReal("-xmax", "X max", "", ctx.xmax, &ctx.xmax, NULL)); PetscCall(PetscOptionsFList("-limit", "Name of flux imiter to use", "", limiters, lname, lname, sizeof(lname), NULL)); PetscCall(PetscOptionsFList("-physics", "Name of physics model to use", "", physics, physname, physname, sizeof(physname), NULL)); PetscCall(PetscOptionsInt("-draw", "Draw solution vector, bitwise OR of (1=initial,2=final,4=final error)", "", draw, &draw, NULL)); PetscCall(PetscOptionsString("-view_final", "Write final solution in ASCII MATLAB format to given file name", "", final_fname, final_fname, sizeof(final_fname), &view_final)); PetscCall(PetscOptionsInt("-initial", "Initial condition (depends on the physics)", "", ctx.initial, &ctx.initial, NULL)); PetscCall(PetscOptionsBool("-exact", "Compare errors with exact solution", "", ctx.exact, &ctx.exact, NULL)); PetscCall(PetscOptionsBool("-simulation", "Compare errors with reference solution", "", ctx.simulation, &ctx.simulation, NULL)); PetscCall(PetscOptionsReal("-cfl", "CFL number to time step at", "", ctx.cfl, &ctx.cfl, NULL)); PetscCall(PetscOptionsEnum("-bc_type", "Boundary condition", "", FVBCTypes, (PetscEnum)ctx.bctype, (PetscEnum *)&ctx.bctype, NULL)); PetscCall(PetscOptionsInt("-hratio", "Spacing ratio", "", ctx.hratio, &ctx.hratio, NULL)); PetscOptionsEnd(); /* Choose the limiter from the list of registered limiters */ PetscCall(PetscFunctionListFind(limiters, lname, &ctx.limit2)); PetscCheck(ctx.limit2, PETSC_COMM_SELF, PETSC_ERR_ARG_UNKNOWN_TYPE, "Limiter '%s' not found", lname); /* Choose the physics from the list of registered models */ { PetscErrorCode (*r)(FVCtx *); PetscCall(PetscFunctionListFind(physics, physname, &r)); PetscCheck(r, PETSC_COMM_SELF, PETSC_ERR_ARG_UNKNOWN_TYPE, "Physics '%s' not found", physname); /* Create the physics, will set the number of fields and their names */ PetscCall((*r)(&ctx)); } /* Create a DMDA to manage the parallel grid */ PetscCall(DMDACreate1d(comm, DM_BOUNDARY_PERIODIC, 50, ctx.physics2.dof, 2, NULL, &da)); PetscCall(DMSetFromOptions(da)); PetscCall(DMSetUp(da)); /* Inform the DMDA of the field names provided by the physics. */ /* The names will be shown in the title bars when run with -ts_monitor_draw_solution */ for (i = 0; i < ctx.physics2.dof; i++) PetscCall(DMDASetFieldName(da, i, ctx.physics2.fieldname[i])); PetscCall(DMDAGetInfo(da, 0, &Mx, 0, 0, 0, 0, 0, &dof, 0, 0, 0, 0, 0)); PetscCall(DMDAGetCorners(da, &xs, 0, 0, &xm, 0, 0)); /* Set coordinates of cell centers */ PetscCall(DMDASetUniformCoordinates(da, ctx.xmin + 0.5 * (ctx.xmax - ctx.xmin) / Mx, ctx.xmax + 0.5 * (ctx.xmax - ctx.xmin) / Mx, 0, 0, 0, 0)); /* Allocate work space for the Finite Volume solver (so it doesn't have to be reallocated on each function evaluation) */ PetscCall(PetscMalloc4(dof * dof, &ctx.R, dof * dof, &ctx.Rinv, 2 * dof, &ctx.cjmpLR, 1 * dof, &ctx.cslope)); PetscCall(PetscMalloc3(2 * dof, &ctx.uLR, dof, &ctx.flux, dof, &ctx.speeds)); PetscCall(PetscMalloc1(2 * dof, &ctx.ub)); /* Create a vector to store the solution and to save the initial state */ PetscCall(DMCreateGlobalVector(da, &X)); PetscCall(VecDuplicate(X, &X0)); PetscCall(VecDuplicate(X, &R)); /* create index for slow parts and fast parts, count_slow + count_fast = Mx, counts_slow*hs = 0.5, counts_fast*hf = 0.5 */ count_slow = Mx * 3 / (3 + ctx.hratio); // compute Mx / (1.0 + ctx.hratio / 3.0); PetscCheck(count_slow % 2 == 0, PETSC_COMM_WORLD, PETSC_ERR_USER, "Please adjust grid size Mx (-da_grid_x) and hratio (-hratio) so that Mx/(1+hratio/3) is even"); count_fast = Mx - count_slow; ctx.sf = count_slow / 2; ctx.fs = ctx.sf + count_fast; PetscCall(PetscMalloc1(xm * dof, &index_slow)); PetscCall(PetscMalloc1(xm * dof, &index_fast)); PetscCall(PetscMalloc1(8 * dof, &index_slowbuffer)); ctx.lsbwidth = 4; ctx.rsbwidth = 4; for (i = xs; i < xs + xm; i++) { if (i < ctx.sf - ctx.lsbwidth || i > ctx.fs + ctx.rsbwidth - 1) for (k = 0; k < dof; k++) index_slow[islow++] = i * dof + k; else if ((i >= ctx.sf - ctx.lsbwidth && i < ctx.sf) || (i > ctx.fs - 1 && i <= ctx.fs + ctx.rsbwidth - 1)) for (k = 0; k < dof; k++) index_slowbuffer[islowbuffer++] = i * dof + k; else for (k = 0; k < dof; k++) index_fast[ifast++] = i * dof + k; } PetscCall(ISCreateGeneral(PETSC_COMM_WORLD, islow, index_slow, PETSC_COPY_VALUES, &ctx.iss)); PetscCall(ISCreateGeneral(PETSC_COMM_WORLD, ifast, index_fast, PETSC_COPY_VALUES, &ctx.isf)); PetscCall(ISCreateGeneral(PETSC_COMM_WORLD, islowbuffer, index_slowbuffer, PETSC_COPY_VALUES, &ctx.issb)); /* Create a time-stepping object */ PetscCall(TSCreate(comm, &ts)); PetscCall(TSSetDM(ts, da)); PetscCall(TSSetRHSFunction(ts, R, FVRHSFunction_2WaySplit, &ctx)); PetscCall(TSRHSSplitSetIS(ts, "slow", ctx.iss)); PetscCall(TSRHSSplitSetIS(ts, "slowbuffer", ctx.issb)); PetscCall(TSRHSSplitSetIS(ts, "fast", ctx.isf)); PetscCall(TSRHSSplitSetRHSFunction(ts, "slow", NULL, FVRHSFunctionslow_2WaySplit, &ctx)); PetscCall(TSRHSSplitSetRHSFunction(ts, "fast", NULL, FVRHSFunctionfast_2WaySplit, &ctx)); PetscCall(TSRHSSplitSetRHSFunction(ts, "slowbuffer", NULL, FVRHSFunctionslowbuffer_2WaySplit, &ctx)); PetscCall(TSSetType(ts, TSMPRK)); PetscCall(TSSetMaxTime(ts, maxtime)); PetscCall(TSSetExactFinalTime(ts, TS_EXACTFINALTIME_STEPOVER)); /* Compute initial conditions and starting time step */ PetscCall(FVSample_2WaySplit(&ctx, da, 0, X0)); PetscCall(FVRHSFunction_2WaySplit(ts, 0, X0, X, (void *)&ctx)); /* Initial function evaluation, only used to determine max speed */ PetscCall(VecCopy(X0, X)); /* The function value was not used so we set X=X0 again */ PetscCall(TSSetTimeStep(ts, ctx.cfl / ctx.cfl_idt)); PetscCall(TSSetFromOptions(ts)); /* Take runtime options */ PetscCall(SolutionStatsView(da, X, PETSC_VIEWER_STDOUT_WORLD)); { PetscInt steps; PetscScalar mass_initial, mass_final, mass_difference, mass_differenceg; const PetscScalar *ptr_X, *ptr_X0; const PetscReal hs = (ctx.xmax - ctx.xmin) * 3.0 / 4.0 / count_slow; const PetscReal hf = (ctx.xmax - ctx.xmin) / 4.0 / count_fast; PetscCall(TSSolve(ts, X)); PetscCall(TSGetSolveTime(ts, &ptime)); PetscCall(TSGetStepNumber(ts, &steps)); /* calculate the total mass at initial time and final time */ mass_initial = 0.0; mass_final = 0.0; PetscCall(DMDAVecGetArrayRead(da, X0, (void *)&ptr_X0)); PetscCall(DMDAVecGetArrayRead(da, X, (void *)&ptr_X)); for (i = xs; i < xs + xm; i++) { if (i < ctx.sf || i > ctx.fs - 1) { for (k = 0; k < dof; k++) { mass_initial = mass_initial + hs * ptr_X0[i * dof + k]; mass_final = mass_final + hs * ptr_X[i * dof + k]; } } else { for (k = 0; k < dof; k++) { mass_initial = mass_initial + hf * ptr_X0[i * dof + k]; mass_final = mass_final + hf * ptr_X[i * dof + k]; } } } PetscCall(DMDAVecRestoreArrayRead(da, X0, (void *)&ptr_X0)); PetscCall(DMDAVecRestoreArrayRead(da, X, (void *)&ptr_X)); mass_difference = mass_final - mass_initial; PetscCallMPI(MPIU_Allreduce(&mass_difference, &mass_differenceg, 1, MPIU_SCALAR, MPIU_SUM, comm)); PetscCall(PetscPrintf(comm, "Mass difference %g\n", (double)mass_differenceg)); PetscCall(PetscPrintf(comm, "Final time %g, steps %" PetscInt_FMT "\n", (double)ptime, steps)); PetscCall(PetscPrintf(comm, "Maximum allowable stepsize according to CFL %g\n", (double)(1.0 / ctx.cfl_idt))); if (ctx.exact) { PetscReal nrm1 = 0; PetscCall(SolutionErrorNorms_2WaySplit(&ctx, da, ptime, X, &nrm1)); PetscCall(PetscPrintf(comm, "Error ||x-x_e||_1 %g\n", (double)nrm1)); } if (ctx.simulation) { PetscReal nrm1 = 0; PetscViewer fd; char filename[PETSC_MAX_PATH_LEN] = "binaryoutput"; Vec XR; PetscBool flg; const PetscScalar *ptr_XR; PetscCall(PetscOptionsGetString(NULL, NULL, "-f", filename, sizeof(filename), &flg)); PetscCheck(flg, PETSC_COMM_WORLD, PETSC_ERR_USER, "Must indicate binary file with the -f option"); PetscCall(PetscViewerBinaryOpen(PETSC_COMM_WORLD, filename, FILE_MODE_READ, &fd)); PetscCall(VecDuplicate(X0, &XR)); PetscCall(VecLoad(XR, fd)); PetscCall(PetscViewerDestroy(&fd)); PetscCall(VecGetArrayRead(X, &ptr_X)); PetscCall(VecGetArrayRead(XR, &ptr_XR)); for (i = xs; i < xs + xm; i++) { if (i < ctx.sf || i > ctx.fs - 1) for (k = 0; k < dof; k++) nrm1 = nrm1 + hs * PetscAbs(ptr_X[i * dof + k] - ptr_XR[i * dof + k]); else for (k = 0; k < dof; k++) nrm1 = nrm1 + hf * PetscAbs(ptr_X[i * dof + k] - ptr_XR[i * dof + k]); } PetscCall(VecRestoreArrayRead(X, &ptr_X)); PetscCall(VecRestoreArrayRead(XR, &ptr_XR)); PetscCall(PetscPrintf(comm, "Error ||x-x_e||_1 %g\n", (double)nrm1)); PetscCall(VecDestroy(&XR)); } } PetscCall(SolutionStatsView(da, X, PETSC_VIEWER_STDOUT_WORLD)); if (draw & 0x1) PetscCall(VecView(X0, PETSC_VIEWER_DRAW_WORLD)); if (draw & 0x2) PetscCall(VecView(X, PETSC_VIEWER_DRAW_WORLD)); if (draw & 0x4) { Vec Y; PetscCall(VecDuplicate(X, &Y)); PetscCall(FVSample_2WaySplit(&ctx, da, ptime, Y)); PetscCall(VecAYPX(Y, -1, X)); PetscCall(VecView(Y, PETSC_VIEWER_DRAW_WORLD)); PetscCall(VecDestroy(&Y)); } if (view_final) { PetscViewer viewer; PetscCall(PetscViewerASCIIOpen(PETSC_COMM_WORLD, final_fname, &viewer)); PetscCall(PetscViewerPushFormat(viewer, PETSC_VIEWER_ASCII_MATLAB)); PetscCall(VecView(X, viewer)); PetscCall(PetscViewerPopFormat(viewer)); PetscCall(PetscViewerDestroy(&viewer)); } /* Clean up */ PetscCall((*ctx.physics2.destroy)(ctx.physics2.user)); for (i = 0; i < ctx.physics2.dof; i++) PetscCall(PetscFree(ctx.physics2.fieldname[i])); PetscCall(PetscFree(ctx.physics2.bcinflowindex)); PetscCall(PetscFree(ctx.ub)); PetscCall(PetscFree4(ctx.R, ctx.Rinv, ctx.cjmpLR, ctx.cslope)); PetscCall(PetscFree3(ctx.uLR, ctx.flux, ctx.speeds)); PetscCall(VecDestroy(&X)); PetscCall(VecDestroy(&X0)); PetscCall(VecDestroy(&R)); PetscCall(DMDestroy(&da)); PetscCall(TSDestroy(&ts)); PetscCall(ISDestroy(&ctx.iss)); PetscCall(ISDestroy(&ctx.isf)); PetscCall(ISDestroy(&ctx.issb)); PetscCall(PetscFree(index_slow)); PetscCall(PetscFree(index_fast)); PetscCall(PetscFree(index_slowbuffer)); PetscCall(PetscFunctionListDestroy(&limiters)); PetscCall(PetscFunctionListDestroy(&physics)); PetscCall(PetscFinalize()); return 0; } /*TEST build: requires: !complex !single depends: finitevolume1d.c test: suffix: 1 args: -da_grid_x 60 -initial 7 -xmin -1 -xmax 1 -hratio 2 -limit mc -ts_dt 0.025 -ts_max_steps 24 -ts_type mprk -ts_mprk_type 2a22 output_file: output/ex4_1.out test: suffix: 2 args: -da_grid_x 60 -initial 7 -xmin -1 -xmax 1 -hratio 2 -limit mc -ts_dt 0.025 -ts_max_steps 24 -ts_type mprk -ts_mprk_type 2a22 -ts_use_splitrhsfunction 1 output_file: output/ex4_1.out test: suffix: 3 args: -da_grid_x 40 -initial 1 -hratio 2 -limit mc -ts_dt 0.1 -ts_max_steps 24 -ts_max_time 7.0 -ts_type mprk -ts_mprk_type 2a22 -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 0 output_file: output/ex4_3.out test: suffix: 4 nsize: 2 args: -da_grid_x 40 -initial 1 -hratio 2 -limit mc -ts_dt 0.1 -ts_max_steps 24 -ts_max_time 7.0 -ts_type mprk -ts_mprk_type 2a22 -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 1 output_file: output/ex4_3.out test: suffix: 5 nsize: 4 args: -da_grid_x 40 -initial 1 -hratio 2 -limit mc -ts_dt 0.1 -ts_max_steps 24 -ts_max_time 7.0 -ts_type mprk -ts_mprk_type 2a22 -physics shallow -bc_type outflow -xmin 0 -xmax 50 -ts_use_splitrhsfunction 1 output_file: output/ex4_3.out TEST*/