Mercurial > repos > public > sbplib
view +sbp/D1Upwind.m @ 774:66eb4a2bbb72 feature/grids
Remove default scaling of the system.
The scaling doens't seem to help actual solutions. One example that fails in the flexural code.
With large timesteps the solutions seems to blow up. One particular example is profilePresentation
on the tdb_presentation_figures branch with k = 0.0005
author | Jonatan Werpers <jonatan@werpers.com> |
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date | Wed, 18 Jul 2018 15:42:52 -0700 |
parents | e1d11b6a68d8 |
children | 111fcbcff2e9 |
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classdef D1Upwind < sbp.OpSet properties Dp, Dm % SBP operator approximating first derivative H % Norm matrix HI % H^-1 e_l % Left boundary operator e_r % Right boundary operator m % Number of grid points. h % Step size x % grid borrowing % Struct with borrowing limits for different norm matrices end methods function obj = D1Upwind(m,lim,order) x_l = lim{1}; x_r = lim{2}; L = x_r-x_l; obj.h = L/(m-1); obj.x = linspace(x_l,x_r,m)'; switch order case 2 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_2(m,obj.h); case 3 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_3(m,obj.h); case 4 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_4(m,obj.h); case 5 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_5(m,obj.h); case 6 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_6(m,obj.h); case 7 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_7(m,obj.h); case 8 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_8(m,obj.h); case 9 [obj.H, obj.HI, obj.Dp, obj.Dm, obj.e_l, obj.e_r] = ... sbp.implementations.d1_upwind_9(m,obj.h); otherwise error('Invalid operator order %d.',order); end obj.m = m; obj.borrowing = []; end function str = string(obj) str = [class(obj) '_' num2str(obj.order)]; end end end