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view +scheme/Beam.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 | a35ed1d124d3 |
children | 2b1b944deae1 25d0efdb0f75 |
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classdef Beam < scheme.Scheme properties order % Order accuracy for the approximation grid D % non-stabalized scheme operator alpha h H % Discrete norm Hi e_l, e_r d1_l, d1_r d2_l, d2_r d3_l, d3_r gamm delt alphaII alphaIII opt % TODO: Get rid of this and use the interface type instead end methods function obj = Beam(grid, order, alpha, opsGen, opt) default_arg('alpha', -1); % default_arg('opsGen', @sbp.D4); default_arg('opsGen', @sbp.D4Variable); % Supposed to be better opt_default.interface_l.tuning = 1.1; opt_default.interface_l.tau = []; opt_default.interface_l.sig = []; opt_default.interface_r.tuning = 1.1; opt_default.interface_r.tau = []; opt_default.interface_r.sig = []; default_struct('opt', opt_default); if ~isa(grid, 'grid.Cartesian') || grid.D() ~= 1 error('Grid must be 1d cartesian'); end obj.grid = grid; obj.order = order; obj.alpha = alpha; m = grid.m; h = grid.scaling(); x_lim = {grid.x{1}(1), grid.x{1}(end)}; ops = opsGen(m, x_lim, order); D4 = ops.D4; obj.H = ops.H; obj.Hi = ops.HI; obj.e_l = ops.e_l; obj.e_r = ops.e_r; obj.d1_l = ops.d1_l; obj.d1_r = ops.d1_r; obj.d2_l = ops.d2_l; obj.d2_r = ops.d2_r; obj.d3_l = ops.d3_l; obj.d3_r = ops.d3_r; obj.D = alpha*D4; alphaII = ops.borrowing.N.S2/2; alphaIII = ops.borrowing.N.S3/2; obj.gamm = h*alphaII; obj.delt = h^3*alphaIII; obj.alphaII = alphaII; obj.alphaIII = alphaIII; obj.h = h; obj.opt = opt; end % Closure functions return the opertors applied to the own doamin to close the boundary % Penalty functions return the opertors to force the solution. In the case of an interface it returns the operator applied to the other doamin. % boundary is a string specifying the boundary e.g. 'l','r' or 'e','w','n','s'. % type is a string specifying the type of boundary condition if there are several. % neighbour_scheme is an instance of Scheme that should be interfaced to. % neighbour_boundary is a string specifying which boundary to interface to. function [closure, penalty] = boundary_condition(obj,boundary,type) default_arg('type','dn'); [e, d1, d2, d3, s] = obj.get_boundary_ops(boundary); gamm = obj.gamm; delt = obj.delt; % TODO: Can this be simplifed? Can I handle conditions on u on its own, u_x on its own ... switch type case {'dn', 'clamped'} % Dirichlet-neumann boundary condition alpha = obj.alpha; % tau1 < -alpha^2/gamma % tuning = 2; tuning = 1.1; tau1 = tuning * alpha/delt; tau4 = s*alpha; sig2 = tuning * alpha/gamm; sig3 = -s*alpha; tau = tau1*e+tau4*d3; sig = sig2*d1+sig3*d2; closure = obj.Hi*(tau*e' + sig*d1'); penalty{1} = -obj.Hi*tau; penalty{2} = -obj.Hi*sig; case {'free'} a = obj.alpha; tau = s*a*d1; sig = -s*a*e; closure = obj.Hi*(tau*d2' + sig*d3'); penalty{1} = -obj.Hi*tau; penalty{1} = -obj.Hi*sig; case 'e' alpha = obj.alpha; tuning = 1.1; tau1 = tuning * alpha/delt; tau4 = s*alpha; tau = tau1*e+tau4*d3; closure = obj.Hi*tau*e'; penalty = -obj.Hi*tau; case 'd1' alpha = obj.alpha; tuning = 1.1; sig2 = tuning * alpha/gamm; sig3 = -s*alpha; sig = sig2*d1+sig3*d2; closure = obj.Hi*sig*d1'; penalty = -obj.Hi*sig; case 'd2' a = obj.alpha; tau = s*a*d1; closure = obj.Hi*tau*d2'; penalty = -obj.Hi*tau; case 'd3' a = obj.alpha; sig = -s*a*e; closure = obj.Hi*sig*d3'; penalty = -obj.Hi*sig; otherwise % Unknown, boundary condition error('No such boundary condition: type = %s',type); end end function [closure, penalty] = interface(obj,boundary,neighbour_scheme,neighbour_boundary, type) % u denotes the solution in the own domain % v denotes the solution in the neighbour domain [e_u,d1_u,d2_u,d3_u,s_u] = obj.get_boundary_ops(boundary); [e_v,d1_v,d2_v,d3_v,s_v] = neighbour_scheme.get_boundary_ops(neighbour_boundary); alpha_u = obj.alpha; alpha_v = neighbour_scheme.alpha; switch boundary case 'l' interface_opt = obj.opt.interface_l; case 'r' interface_opt = obj.opt.interface_r; end if isempty(interface_opt.tau) && isempty(interface_opt.sig) gamm_u = obj.gamm; delt_u = obj.delt; gamm_v = neighbour_scheme.gamm; delt_v = neighbour_scheme.delt; tuning = interface_opt.tuning; tau1 = ((alpha_u/2)/delt_u + (alpha_v/2)/delt_v)/2*tuning; sig2 = ((alpha_u/2)/gamm_u + (alpha_v/2)/gamm_v)/2*tuning; else h_u = obj.h; h_v = neighbour_scheme.h; switch neighbour_boundary case 'l' neighbour_interface_opt = neighbour_scheme.opt.interface_l; case 'r' neighbour_interface_opt = neighbour_scheme.opt.interface_r; end tau_u = interface_opt.tau; sig_u = interface_opt.sig; tau_v = neighbour_interface_opt.tau; sig_v = neighbour_interface_opt.sig; tau1 = tau_u/h_u^3 + tau_v/h_v^3; sig2 = sig_u/h_u + sig_v/h_v; end tau4 = s_u*alpha_u/2; sig3 = -s_u*alpha_u/2; phi2 = s_u*1/2; psi1 = -s_u*1/2; tau = tau1*e_u + tau4*d3_u; sig = sig2*d1_u + sig3*d2_u ; phi = phi2*d1_u ; psi = psi1*e_u ; closure = obj.Hi*(tau*e_u' + sig*d1_u' + phi*alpha_u*d2_u' + psi*alpha_u*d3_u'); penalty = -obj.Hi*(tau*e_v' + sig*d1_v' + phi*alpha_v*d2_v' + psi*alpha_v*d3_v'); end % Returns the boundary ops and sign for the boundary specified by the string boundary. % The right boundary is considered the positive boundary function [e, d1, d2, d3, s] = get_boundary_ops(obj,boundary) switch boundary case 'l' e = obj.e_l; d1 = obj.d1_l; d2 = obj.d2_l; d3 = obj.d3_l; s = -1; case 'r' e = obj.e_r; d1 = obj.d1_r; d2 = obj.d2_r; d3 = obj.d3_r; s = 1; otherwise error('No such boundary: boundary = %s',boundary); end end function N = size(obj) N = obj.grid.N; end end end