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$$u_{t}+u u_{x}=0$$ $$u(x,0)= \begin{cases} 1 & \text{if}\quad x<0 \ 0 & \text{if}\quad 0<x<1 \ 1 & \text{if}\quad x<1 \end

User124356
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It is the opposite Cauchy problem as in this post. Here we have a shock with speed 1/2 starting at $x=0$ and a rarefaction starting at $x=1$. Therefore, $$ u(x,t) =\left\lbrace \begin{aligned} &1 &&\text{if}\quad x<t/2\\ &0 &&\text{if}\quad t/2<x\le 1\\ &\tfrac{x-1}{t} &&\text{if}\quad 1\le x\le 1+t\\ &1 &&\text{if}\quad x\ge 1+t \end{aligned}\right. $$ for small times $t<t^*$.

The shock wave catches the rarefaction at $t^* = 2$. From this moment, the speed $s'(t)$ of the shock is modified due to the modification of data on the right. Following the Rankine-Hugoniot condition, we have $$ s'(t) = \tfrac{1}{2}\left(1 + \tfrac{s(t)-1}{t}\right) $$ with the initial condition $s(2) = 1$. The shock trajectory satisfies $s(t) = 1+t-\sqrt{2t}$, so that $$ u(x,t) =\left\lbrace \begin{aligned} &1 &&\text{if}\quad x<s(t)\\ &\tfrac{x-1}{t} &&\text{if}\quad s(t)< x\le 1+t\\ &1 &&\text{if}\quad x\ge 1+t \end{aligned}\right. $$ for small times $t>t^*$. One notes that the shock slows down and never overtakes the rarefaction.

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