Mercurial > repos > public > sbplib
comparison +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 |
comparison
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854:18162a0a5bb5 | 1033:037f203b9bf5 |
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1 function [D_rv, D_flux, DvDt, solutionPenalties, residualPenalties] = constructDiffOps(scheme, grid, order, opSet, waveSpeed, BCs, fluxSplitting) | |
2 default_arg('fluxSplitting',[]); | |
3 | |
4 %% DiffOps for solution vector | |
5 [D, solutionPenalties] = constructTotalFluxDiffOp(scheme, grid, order, opSet, waveSpeed, BCs, fluxSplitting); | |
6 D2 = constructSymmetricD2Operator(grid, order, opSet); | |
7 D_rv = @(v,viscosity)(D + D2(viscosity))*v; | |
8 | |
9 %% DiffOps for residual viscosity | |
10 [D_flux, residualPenalties] = constructTotalFluxDiffOp(scheme, grid, max(order-2,2), opSet, waveSpeed, BCs, fluxSplitting); | |
11 % DiffOp for flux in residual viscosity. Due to sign conventions of the implemnted schemes, we need to | |
12 % change the sign. | |
13 D_flux = -D_flux; | |
14 D_flux = @(v) D_flux*v; | |
15 % DiffOp for time derivative in residual viscosity | |
16 DvDt = @(v)D*v; | |
17 end | |
18 | |
19 function [D, penalties] = constructTotalFluxDiffOp(scheme, grid, order, opSet, waveSpeed, BCs, fluxSplitting) | |
20 if isequal(opSet, @sbp.D1Upwind) | |
21 diffOp = scheme(grid, order, opSet, waveSpeed, fluxSplitting); | |
22 else | |
23 diffOp = scheme(grid, order, opSet, waveSpeed); | |
24 end | |
25 [D, penalties] = addClosuresToDiffOp(diffOp, BCs); | |
26 end | |
27 | |
28 function [D, penalties] = addClosuresToDiffOp(diffOp, BCs) | |
29 D = diffOp.D; | |
30 penalties = cell(size(BCs)); | |
31 for i = 1:size(BCs,1) | |
32 for j = 1:size(BCs,2) | |
33 [closure, penalties{i,j}] = diffOp.boundary_condition(BCs{i,j}.boundary, BCs{i,j}.type); | |
34 D = D + closure; | |
35 end | |
36 end | |
37 end | |
38 | |
39 function D2 = constructSymmetricD2Operator(grid, order, opSet) | |
40 % TODO: | |
41 % Currently only implemented for upwind operators. | |
42 % Remove this part once the time-dependent D2 operator is implemented for other opSets | |
43 % or if it is decided that it should only be supported for upwind operators. | |
44 assert(isequal(opSet,@sbp.D1Upwind)) | |
45 | |
46 m = grid.size(); | |
47 ops = cell(grid.D(),1); | |
48 I = cell(grid.D(),1); | |
49 for i = 1:grid.D() | |
50 lim = {grid.x{i}(1), grid.x{i}(end)}; | |
51 ops{i} = opSet(m(i), lim, order); | |
52 I{i} = speye(m(i)); | |
53 end | |
54 | |
55 % TBD: How is this generalized to a loop over dimensions or similar? | |
56 switch grid.D() | |
57 case 1 | |
58 e_r = ops{1}.e_r; | |
59 e_l = ops{1}.e_l; | |
60 Dm = ops{1}.Dm; | |
61 Dp = ops{1}.Dp; | |
62 Hi = ops{1}.HI; | |
63 B = e_r*e_r' - e_l*e_l'; | |
64 D2 = @(viscosity) Dm*spdiag(viscosity)*Dp-Hi*(B*spdiag(viscosity)*Dp); | |
65 case 2 | |
66 e_e = kron(ops{1}.e_r,I{2}); | |
67 e_w = kron(ops{1}.e_l,I{2}); | |
68 Dm_x = kron(ops{1}.Dm,I{2}); | |
69 Dp_x = kron(ops{1}.Dp,I{2}); | |
70 H_x = kron(ops{1}.HI,I{2}); | |
71 B_x = e_e*e_e' - e_w*e_w'; | |
72 D2_x = @(viscosity) Dm_x*spdiag(viscosity)*Dp_x-H_x*(B_x*spdiag(viscosity)*Dp_x); | |
73 | |
74 e_n = kron(I{1},ops{2}.e_r); | |
75 e_s = kron(I{1},ops{2}.e_l); | |
76 Dm_y = kron(I{1},ops{2}.Dm); | |
77 Dp_y = kron(I{1},ops{2}.Dp); | |
78 H_y = kron(I{1},ops{2}.HI); | |
79 B_y = e_n*e_n' - e_s*e_s'; | |
80 D2_y = @(viscosity) Dm_y*spdiag(viscosity)*Dp_y-H_y*(B_y*spdiag(viscosity)*Dp_y); | |
81 D2 = @(viscosity)D2_x(viscosity) + D2_y(viscosity); | |
82 otherwise | |
83 error('3D not yet implemented') | |
84 end | |
85 end |