Mercurial > repos > public > sbplib
diff +rv/constructDiffOps.m @ 1033:037f203b9bf5 feature/burgers1d
Merge with branch feature/advectioRV to utilize the +rv package
author | Vidar Stiernström <vidar.stiernstrom@it.uu.se> |
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date | Thu, 17 Jan 2019 10:44:12 +0100 |
parents | 44c3ea38097e |
children | 1a5c8723c9be 2d7ba44340d0 |
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--- /dev/null Thu Jan 01 00:00:00 1970 +0000 +++ b/+rv/constructDiffOps.m Thu Jan 17 10:44:12 2019 +0100 @@ -0,0 +1,85 @@ +function [D_rv, D_flux, DvDt, solutionPenalties, residualPenalties] = constructDiffOps(scheme, grid, order, opSet, waveSpeed, BCs, fluxSplitting) + default_arg('fluxSplitting',[]); + + %% DiffOps for solution vector + [D, solutionPenalties] = constructTotalFluxDiffOp(scheme, grid, order, opSet, waveSpeed, BCs, fluxSplitting); + D2 = constructSymmetricD2Operator(grid, order, opSet); + D_rv = @(v,viscosity)(D + D2(viscosity))*v; + + %% DiffOps for residual viscosity + [D_flux, residualPenalties] = constructTotalFluxDiffOp(scheme, grid, max(order-2,2), opSet, waveSpeed, BCs, fluxSplitting); + % DiffOp for flux in residual viscosity. Due to sign conventions of the implemnted schemes, we need to + % change the sign. + D_flux = -D_flux; + D_flux = @(v) D_flux*v; + % DiffOp for time derivative in residual viscosity + DvDt = @(v)D*v; +end + +function [D, penalties] = constructTotalFluxDiffOp(scheme, grid, order, opSet, waveSpeed, BCs, fluxSplitting) + if isequal(opSet, @sbp.D1Upwind) + diffOp = scheme(grid, order, opSet, waveSpeed, fluxSplitting); + else + diffOp = scheme(grid, order, opSet, waveSpeed); + end + [D, penalties] = addClosuresToDiffOp(diffOp, BCs); +end + +function [D, penalties] = addClosuresToDiffOp(diffOp, BCs) + D = diffOp.D; + penalties = cell(size(BCs)); + for i = 1:size(BCs,1) + for j = 1:size(BCs,2) + [closure, penalties{i,j}] = diffOp.boundary_condition(BCs{i,j}.boundary, BCs{i,j}.type); + D = D + closure; + end + end +end + +function D2 = constructSymmetricD2Operator(grid, order, opSet) + % TODO: + % Currently only implemented for upwind operators. + % Remove this part once the time-dependent D2 operator is implemented for other opSets + % or if it is decided that it should only be supported for upwind operators. + assert(isequal(opSet,@sbp.D1Upwind)) + + m = grid.size(); + ops = cell(grid.D(),1); + I = cell(grid.D(),1); + for i = 1:grid.D() + lim = {grid.x{i}(1), grid.x{i}(end)}; + ops{i} = opSet(m(i), lim, order); + I{i} = speye(m(i)); + end + + % TBD: How is this generalized to a loop over dimensions or similar? + switch grid.D() + case 1 + e_r = ops{1}.e_r; + e_l = ops{1}.e_l; + Dm = ops{1}.Dm; + Dp = ops{1}.Dp; + Hi = ops{1}.HI; + B = e_r*e_r' - e_l*e_l'; + D2 = @(viscosity) Dm*spdiag(viscosity)*Dp-Hi*(B*spdiag(viscosity)*Dp); + case 2 + e_e = kron(ops{1}.e_r,I{2}); + e_w = kron(ops{1}.e_l,I{2}); + Dm_x = kron(ops{1}.Dm,I{2}); + Dp_x = kron(ops{1}.Dp,I{2}); + H_x = kron(ops{1}.HI,I{2}); + B_x = e_e*e_e' - e_w*e_w'; + D2_x = @(viscosity) Dm_x*spdiag(viscosity)*Dp_x-H_x*(B_x*spdiag(viscosity)*Dp_x); + + e_n = kron(I{1},ops{2}.e_r); + e_s = kron(I{1},ops{2}.e_l); + Dm_y = kron(I{1},ops{2}.Dm); + Dp_y = kron(I{1},ops{2}.Dp); + H_y = kron(I{1},ops{2}.HI); + B_y = e_n*e_n' - e_s*e_s'; + D2_y = @(viscosity) Dm_y*spdiag(viscosity)*Dp_y-H_y*(B_y*spdiag(viscosity)*Dp_y); + D2 = @(viscosity)D2_x(viscosity) + D2_y(viscosity); + otherwise + error('3D not yet implemented') + end +end \ No newline at end of file