Mercurial > repos > public > sbplib
view +sbp/D1Upwind.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> |
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date | Thu, 17 Jan 2019 10:25:06 +0100 |
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