function [u,u_exact,x,t] = lax_wendroff(f,t_0,t_f,M,N)% define the mesh in space
dx = 2*pi/N;x = 0:dx:2*pi;x = x';% define the mesh in time
dt = (t_f-t_0)/M;t = t_0:dt:t_f;c = 1/2;% display('this number should be between -1 and 1 for stability:')
mu = c*dt/dx;% choose the wave number of the initial data and give its decay rate
u= zeros(N+1,M+1);u(:,1) = f(x);u_exact(:,1) = u(:,1);% I want to do the Lax Wendroff scheme:
%
% u_new(j) = u_old(j) - (mu/2)*(u_old(j+1)-u_old(j-1))
% + (mu^2/2)*(u_old(j-1)-2*u_old(j)+u_old(j+1))
for j=1:M for k=2:N u(k,j+1) = u(k,j) - (mu/2)*(u(k+1,j)-u(k-1,j)) + (mu^2/2)*(u(k+1,j)-2*u(k,j)+u(k-1,j)); end % I code in the exact values at the endpoints.
u(1,j+1)=1; u(N+1,j+1)=0; X = x-c*t(j+1); u_exact(:,j+1) = f(X);endendfunction y = f(x)% for step function initial data:
y = x<=(pi-1);end% [u,err,x,t] = lax_wendroff(@f,t_0,t_f,M,N)
%% solves the heat equation u_t + u_x = 0 [0,2*pi]
%% If I'm going to use the FFT to analyse the solution then I'd like to take
% N of the form 2^k. This will also have the advantage of making sure there's
% always a meshpoint at x = pi
%% f.m is the function that contains the initial data
MATLAB: I want to link the below two functions..hope somebody can help ..
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