// Copyright (c) 2017-2022, Lawrence Livermore National Security, LLC and other CEED contributors. // All Rights Reserved. See the top-level LICENSE and NOTICE files for details. // // SPDX-License-Identifier: BSD-2-Clause // // This file is part of CEED: http://github.com/ceed /// @file /// Advection initial condition and operator for Navier-Stokes example using PETSc #ifndef advection_h #define advection_h #include #include #include "advection_generic.h" #include "advection_types.h" #include "newtonian_state.h" #include "newtonian_types.h" #include "stabilization_types.h" #include "utils.h" // ***************************************************************************** // This QFunction sets the initial conditions for 3D advection // ***************************************************************************** CEED_QFUNCTION(ICsAdvection)(void *ctx, CeedInt Q, const CeedScalar *const *in, CeedScalar *const *out) { const CeedScalar(*X)[CEED_Q_VLA] = (const CeedScalar(*)[CEED_Q_VLA])in[0]; CeedScalar(*q0)[CEED_Q_VLA] = (CeedScalar(*)[CEED_Q_VLA])out[0]; CeedPragmaSIMD for (CeedInt i = 0; i < Q; i++) { const CeedScalar x[] = {X[0][i], X[1][i], X[2][i]}; CeedScalar q[5] = {0.}; Exact_AdvectionGeneric(3, 0., x, 5, q, ctx); for (CeedInt j = 0; j < 5; j++) q0[j][i] = q[j]; } return 0; } // ***************************************************************************** // This QFunction implements the following formulation of the advection equation // // This is 3D advection given in two formulations based upon the weak form. // // State Variables: q = ( rho, U1, U2, U3, E ) // rho - Mass Density // Ui - Momentum Density , Ui = rho ui // E - Total Energy Density // // Advection Equation: // dE/dt + div( E u ) = 0 // ***************************************************************************** CEED_QFUNCTION(Advection)(void *ctx, CeedInt Q, const CeedScalar *const *in, CeedScalar *const *out) { // Inputs const CeedScalar(*q)[CEED_Q_VLA] = (const CeedScalar(*)[CEED_Q_VLA])in[0]; const CeedScalar(*dq)[5][CEED_Q_VLA] = (const CeedScalar(*)[5][CEED_Q_VLA])in[1]; const CeedScalar(*q_data) = in[2]; // Outputs CeedScalar(*v)[CEED_Q_VLA] = (CeedScalar(*)[CEED_Q_VLA])out[0]; CeedScalar(*dv)[5][CEED_Q_VLA] = (CeedScalar(*)[5][CEED_Q_VLA])out[1]; // Context AdvectionContext context = (AdvectionContext)ctx; const CeedScalar CtauS = context->CtauS; const CeedScalar strong_form = context->strong_form; // Quadrature Point Loop CeedPragmaSIMD for (CeedInt i = 0; i < Q; i++) { // Setup // -- Interp in const CeedScalar rho = q[0][i]; const CeedScalar u[3] = {q[1][i] / rho, q[2][i] / rho, q[3][i] / rho}; const CeedScalar E = q[4][i]; // -- Grad in const CeedScalar drho[3] = {dq[0][0][i], dq[1][0][i], dq[2][0][i]}; const CeedScalar du[3][3] = { {(dq[0][1][i] - drho[0] * u[0]) / rho, (dq[1][1][i] - drho[1] * u[0]) / rho, (dq[2][1][i] - drho[2] * u[0]) / rho}, {(dq[0][2][i] - drho[0] * u[1]) / rho, (dq[1][2][i] - drho[1] * u[1]) / rho, (dq[2][2][i] - drho[2] * u[1]) / rho}, {(dq[0][3][i] - drho[0] * u[2]) / rho, (dq[1][3][i] - drho[1] * u[2]) / rho, (dq[2][3][i] - drho[2] * u[2]) / rho} }; const CeedScalar dE[3] = {dq[0][4][i], dq[1][4][i], dq[2][4][i]}; CeedScalar wdetJ, dXdx[3][3]; QdataUnpack_3D(Q, i, q_data, &wdetJ, dXdx); // The Physics // Note with the order that du was filled and the order that dXdx was filled // du[j][k]= du_j / dX_K (note cap K to be clear this is u_{j,xi_k}) // dXdx[k][j] = dX_K / dx_j // X_K=Kth reference element coordinate (note cap X and K instead of xi_k} // x_j and u_j are jth physical position and velocity components // No Change in density or momentum for (CeedInt f = 0; f < 4; f++) { for (CeedInt j = 0; j < 3; j++) dv[j][f][i] = 0; v[f][i] = 0; } // -- Total Energy // Evaluate the strong form using div(E u) = u . grad(E) + E div(u) // or in index notation: (u_j E)_{,j} = u_j E_j + E u_{j,j} CeedScalar div_u = 0, u_dot_grad_E = 0; for (CeedInt j = 0; j < 3; j++) { CeedScalar dEdx_j = 0; for (CeedInt k = 0; k < 3; k++) { div_u += du[j][k] * dXdx[k][j]; // u_{j,j} = u_{j,K} X_{K,j} dEdx_j += dE[k] * dXdx[k][j]; } u_dot_grad_E += u[j] * dEdx_j; } CeedScalar strong_conv = E * div_u + u_dot_grad_E; // Weak Galerkin convection term: dv \cdot (E u) for (CeedInt j = 0; j < 3; j++) dv[j][4][i] = (1 - strong_form) * wdetJ * E * (u[0] * dXdx[j][0] + u[1] * dXdx[j][1] + u[2] * dXdx[j][2]); v[4][i] = 0; // Strong Galerkin convection term: - v div(E u) v[4][i] = -strong_form * wdetJ * strong_conv; // Stabilization requires a measure of element transit time in the velocity // field u. CeedScalar uX[3]; for (CeedInt j = 0; j < 3; j++) uX[j] = dXdx[j][0] * u[0] + dXdx[j][1] * u[1] + dXdx[j][2] * u[2]; const CeedScalar TauS = CtauS / sqrt(Dot3(uX, uX)); for (CeedInt j = 0; j < 3; j++) dv[j][4][i] -= wdetJ * TauS * strong_conv * uX[j]; } // End Quadrature Point Loop return 0; } // ***************************************************************************** // This QFunction implements 3D (mentioned above) with implicit time stepping method // ***************************************************************************** CEED_QFUNCTION(IFunction_Advection)(void *ctx, CeedInt Q, const CeedScalar *const *in, CeedScalar *const *out) { const CeedScalar(*q)[CEED_Q_VLA] = (const CeedScalar(*)[CEED_Q_VLA])in[0]; const CeedScalar(*Grad_q)[5][CEED_Q_VLA] = (const CeedScalar(*)[5][CEED_Q_VLA])in[1]; const CeedScalar(*q_dot)[CEED_Q_VLA] = (const CeedScalar(*)[CEED_Q_VLA])in[2]; const CeedScalar(*q_data) = in[3]; CeedScalar(*v)[CEED_Q_VLA] = (CeedScalar(*)[CEED_Q_VLA])out[0]; CeedScalar(*Grad_v)[5][CEED_Q_VLA] = (CeedScalar(*)[5][CEED_Q_VLA])out[1]; CeedScalar *jac_data = out[2]; AdvectionContext context = (AdvectionContext)ctx; const CeedScalar CtauS = context->CtauS; const CeedScalar strong_form = context->strong_form; const CeedScalar zeros[14] = {0.}; NewtonianIdealGasContext gas; struct NewtonianIdealGasContext_ gas_struct = {0}; gas = &gas_struct; CeedPragmaSIMD for (CeedInt i = 0; i < Q; i++) { const CeedScalar qi[5] = {q[0][i], q[1][i], q[2][i], q[3][i], q[4][i]}; const State s = StateFromU(gas, qi); CeedScalar wdetJ, dXdx[3][3]; QdataUnpack_3D(Q, i, q_data, &wdetJ, dXdx); State grad_s[3]; StatePhysicalGradientFromReference(Q, i, gas, s, STATEVAR_CONSERVATIVE, (CeedScalar *)Grad_q, dXdx, grad_s); const CeedScalar Grad_E[3] = {grad_s[0].U.E_total, grad_s[1].U.E_total, grad_s[2].U.E_total}; for (CeedInt f = 0; f < 4; f++) { for (CeedInt j = 0; j < 3; j++) Grad_v[j][f][i] = 0; // No Change in density or momentum v[f][i] = wdetJ * q_dot[f][i]; // K Mass/transient term } CeedScalar div_u = 0; for (CeedInt j = 0; j < 3; j++) { for (CeedInt k = 0; k < 3; k++) { div_u += grad_s[k].Y.velocity[j]; } } CeedScalar strong_conv = s.U.E_total * div_u + Dot3(s.Y.velocity, Grad_E); CeedScalar strong_res = q_dot[4][i] + strong_conv; v[4][i] = wdetJ * q_dot[4][i]; // transient part (ALWAYS) if (strong_form) { // Strong Galerkin convection term: v div(E u) v[4][i] += wdetJ * strong_conv; } else { // Weak Galerkin convection term: -dv \cdot (E u) for (CeedInt j = 0; j < 3; j++) Grad_v[j][4][i] = -wdetJ * s.U.E_total * (s.Y.velocity[0] * dXdx[j][0] + s.Y.velocity[1] * dXdx[j][1] + s.Y.velocity[2] * dXdx[j][2]); } // Stabilization requires a measure of element transit time in the velocity field u. CeedScalar uX[3] = {0.}; MatVec3(dXdx, s.Y.velocity, CEED_NOTRANSPOSE, uX); const CeedScalar TauS = CtauS / sqrt(Dot3(uX, uX)); for (CeedInt j = 0; j < 3; j++) switch (context->stabilization) { case STAB_NONE: break; case STAB_SU: Grad_v[j][4][i] += wdetJ * TauS * strong_conv * uX[j]; break; case STAB_SUPG: Grad_v[j][4][i] += wdetJ * TauS * strong_res * uX[j]; break; } StoredValuesPack(Q, i, 0, 14, zeros, jac_data); } return 0; } // ***************************************************************************** // This QFunction implements consistent outflow and inflow BCs // for 3D advection // // Inflow and outflow faces are determined based on sign(dot(wind, normal)): // sign(dot(wind, normal)) > 0 : outflow BCs // sign(dot(wind, normal)) < 0 : inflow BCs // // Outflow BCs: // The validity of the weak form of the governing equations is extended to the outflow and the current values of E are applied. // // Inflow BCs: // A prescribed Total Energy (E_wind) is applied weakly. // ***************************************************************************** CEED_QFUNCTION(Advection_InOutFlow)(void *ctx, CeedInt Q, const CeedScalar *const *in, CeedScalar *const *out) { // Inputs const CeedScalar(*q)[CEED_Q_VLA] = (const CeedScalar(*)[CEED_Q_VLA])in[0]; const CeedScalar(*q_data_sur) = in[2]; // Outputs CeedScalar(*v)[CEED_Q_VLA] = (CeedScalar(*)[CEED_Q_VLA])out[0]; AdvectionContext context = (AdvectionContext)ctx; const CeedScalar E_wind = context->E_wind; const CeedScalar strong_form = context->strong_form; const bool is_implicit = context->implicit; // Quadrature Point Loop CeedPragmaSIMD for (CeedInt i = 0; i < Q; i++) { // Setup // -- Interp in const CeedScalar rho = q[0][i]; const CeedScalar u[3] = {q[1][i] / rho, q[2][i] / rho, q[3][i] / rho}; const CeedScalar E = q[4][i]; CeedScalar wdetJb, norm[3]; QdataBoundaryUnpack_3D(Q, i, q_data_sur, &wdetJb, NULL, norm); wdetJb *= is_implicit ? -1. : 1.; // Normal velocity const CeedScalar u_normal = norm[0] * u[0] + norm[1] * u[1] + norm[2] * u[2]; // No Change in density or momentum for (CeedInt j = 0; j < 4; j++) { v[j][i] = 0; } // Implementing in/outflow BCs if (u_normal > 0) { // outflow v[4][i] = -(1 - strong_form) * wdetJb * E * u_normal; } else { // inflow v[4][i] = -(1 - strong_form) * wdetJb * E_wind * u_normal; } } // End Quadrature Point Loop return 0; } // ***************************************************************************** #endif // advection_h