Wave Equation Consider the Lax-Friedrichs scheme below for the PDE \(v_t+cv_x=0\), where you may assume that \(c>0\): \[ u_j^{n+1}=\frac {1}{2}(u_{j-1}^n+u_{j+1}^n) -\frac {ck}{2h}(u_{j+1}^n-u_{j-1}^n), \] where \(h\) is the spacestep and \(k\) is the timestep. Note that the scheme can also be written \[ u_j^{n+1}=u_j^n-\frac {ck}{2h}(u_{j+1}^n-u_{j-1}^n) +\frac {1}{2}(u_{j-1}^n-2u_j^n+u_{j+1}^n). \]
a) Analyze the stability of this scheme in terms of \(\alpha =\frac {ck}{h}\).
b) Recall that a modified equation for a scheme is the PDE satisfied, to a certain order, by a smooth solution \(u(x,t)\) of the difference scheme. To zeroth order in \(k\) and \(h\), the modified equation for the Lax-Friedrichs scheme is \(u_t+cu_x=0\). Derive the modified equation through terms of first order in \(k\) and \(h\). You may assume that \(\alpha \) is constant. Does this modified equation predict the same stability condition as your analysis in part a)? Explain your answer. What does the modified equation suggest about the numerical solution that will be obtained for the step-function initial data \(u(x,0)=1\) for \(x\le 0\) and \(u(x,0)=0\) for \(x>0\)?