Scalar conservation law in a bounded domain with strong source at boundary

Lu Xu
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Abstract

We consider a scalar conservation law with source in a bounded open interval \(\Omega \subseteq \mathbb R\). The equation arises from the macroscopic evolution of an interacting particle system. The source term models an external effort driving the solution to a given function \(\varrho \) with an intensity function \(V:\Omega \rightarrow \mathbb R_+\) that grows to infinity at \(\partial \Omega \). We define the entropy solution \(u \in L^\infty \) and prove the uniqueness. When V is integrable, u satisfies the boundary conditions introduced by F. Otto (C. R. Acad. Sci. Paris, 322(1):729–734, 1996), which allows the solution to attain values at \(\partial \Omega \) different from the given boundary data. When the integral of V blows up, u satisfies an energy estimate and presents essential continuity at \(\partial \Omega \) in a weak sense.

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边界强源有界域中的标量守恒定律
我们考虑一个标量守恒定律,其源点位于一个有界的开放区间(\Omega \subseteq \mathbb R\ )。该方程源于相互作用粒子系统的宏观演化。源项模拟的是一种外部作用,它将解驱动为一个给定的函数(\varrho \),其强度函数(V:\Omega \rightarrow \mathbb R_+\)在\(\partial \Omega \)处增长到无穷大。我们定义了熵解 \(u \in L^\infty \) 并证明了其唯一性。当 V 可积分时,u 满足 F. Otto 引入的边界条件(C. R. Acad.Sci. Paris, 322(1):729-734, 1996),它允许解在不同于给定边界数据的 \(partial \Omega \)处取值。当 V 的积分爆炸时,u 满足能量估计,并在\(\partial \Omega \)处呈现弱意义上的基本连续性。
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