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view +time/SBPInTimeSecondOrderFormImplicit.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 | 66eb4a2bbb72 |
children | 8894e9c49e40 |
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classdef SBPInTimeSecondOrderFormImplicit < time.Timestepper properties A, B, C, f AA, BB, ff n t k firstOrderTimeStepper end methods % Solves A*u_tt + B*u_t + C*u = f(t) % A, B can either both be constants or both be function handles, % They can also be omitted by setting them equal to the empty matrix. function obj = SBPInTimeSecondOrderFormImplicit(A, B, C, f, k, t0, v0, v0t, do_scaling, TYPE, order, blockSize) default_arg('f', []); default_arg('TYPE', []); default_arg('order', []); default_arg('blockSize',[]); default_arg('do_scaling', false); m = length(v0); default_arg('A', speye(m, m)); default_arg('B', sparse(m, m)); default_arg('C', sparse(m, m)); I = speye(m); O = sparse(m,m); % Rewrite to % AA*w_t = BB*w + ff(t); obj.AA = [ I, O; O, A; ]; obj.BB = [ O, I; -C, -B; ]; if ~isempty(f) obj.ff = @(t)[ sparse(m,1); f(t); ]; else obj.ff = @(t) sparse(2*m,1); end w0 = [v0; v0t]; obj.k = k; obj.t = t0; obj.n = 0; if do_scaling scaling = [ones(m,1); sqrt(diag(C))]; obj.firstOrderTimeStepper = time.SBPInTimeScaled(obj.AA, obj.BB, obj.ff, obj.k, obj.t, w0, scaling, TYPE, order, blockSize); else obj.firstOrderTimeStepper = time.SBPInTimeImplicitFormulation(obj.AA, obj.BB, obj.ff, obj.k, obj.t, w0, TYPE, order, blockSize); end end function [v,t] = getV(obj) w = obj.firstOrderTimeStepper.getV(); v = w(1:end/2); t = obj.t; end function [vt,t] = getVt(obj) w = obj.firstOrderTimeStepper.getV(); vt = w(end/2+1:end); t = obj.t; end function obj = step(obj) obj.firstOrderTimeStepper.step(); obj.t = obj.firstOrderTimeStepper.t; obj.n = obj.firstOrderTimeStepper.n; end end end