Weak solutions of initial value problem of conservation laws with $L^{\infty}$ initial data

analysisfunctional-analysishamilton-jacobi-equationpartial differential equations

QUESTION:If initial data $u_0 \in L^{\infty}$ In which sense weak solution of scalar conservation laws $u_t+f(u)_x=0$ $u(x,0)=u_0(x)$ takes initial data?

Explanation:

HYPERBOLIC SYSTEMS OF CONSERVATION LAWS, chapter 2 by Godlewski and Raviart theorem 3.1 states

"if $u_0 \in L^{\infty}(\mathbb{R}^d) \cap L^{1}(\mathbb{R}^d) \cap BV(\mathbb{R}^d)$ then the initial value problem has an entropy solution $u \in L^{\infty}(\mathbb{R}^d \times (0,+\infty)) \cap B(0,T;L^{\mathbb{R}^d})$, which satisfies

$\int_{\mathbb{R}^d} |u(x,t_1)-u(x,t_2)| \,dx \leq CTV(u_0)|t_1-t_2|$ for all $t_1,t_2 \geq 0$"

i.e $u(\cdot,t) \rightarrow u_0$ in $L^1$

Now if we assume $u_0$ to be in just $L^\infty(\mathbb{R^d})$ can we say
$u(\cdot,t) \rightarrow u_0$ in $L^1_{loc} (\mathbb{R^d})$?

if not in which sense $u(\cdot,t) \rightarrow u_0$

Best Answer

As far as I understand for $L^{\infty}$ solutions, the initial data is taken in $L^1_{loc}$ sense. Please correct me if I am wrong.

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