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view +time/Rk4SecondOrderNonlin.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 | c6fcee3fcf1b |
children |
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classdef Rk4SecondOrderNonlin < time.Timestepper properties F k t w m D E S n end methods function obj = Rk4SecondOrderNonlin(D, E, S, k, t0, v0, v0t) default_arg('S',0); default_arg('E',0); if isnumeric(S) S = @(v,t)S; end if isnumeric(E) E = @(v)E; end obj.k = k; obj.t = t0; obj.w = [v0; v0t]; m = length(v0); function wt = F(w,t) v = w(1:m); vt = w(m+1:end); % Def: w = [v; vt] wt(1:m,1) = vt; wt(m+1:2*m,1) = D(v)*v + E(v)*vt + S(v,t); end obj.F = @F; obj.D = D; obj.E = E; obj.S = S; obj.m = m; obj.n = 0; end function [v,t] = getV(obj) v = obj.w(1:end/2); t = obj.t; end function [vt,t] = getVt(obj) vt = obj.w(end/2+1:end); t = obj.t; end function obj = step(obj) obj.w = time.rk.rungekutta_4(obj.w, obj.t, obj.k, obj.F); obj.t = obj.t + obj.k; obj.n = obj.n + 1; end end methods (Static) function k = getTimeStep(lambda) k = rk4.get_rk4_time_step(lambda); end end end