view +rv/constructDiffOps.m @ 1031:2ef20d00b386 feature/advectionRV

For easier comparison, return both the first order and residual viscosity when evaluating the residual. Add the first order and residual viscosity to the state of the RungekuttaRV time steppers
author Vidar Stiernström <vidar.stiernstrom@it.uu.se>
date Thu, 17 Jan 2019 10:25:06 +0100
parents 44c3ea38097e
children 1a5c8723c9be 2d7ba44340d0
line wrap: on
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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