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arXiv 2304.02429math.AP
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三维扰动下柱形跨声速激波解的存在性与稳定性

Existence and stability of cylindrical transonic shock solutions under three dimensional perturbations

Shangkun Weng, Zhouping Xin

AI总结:

本文研究三维入流与出口压力扰动下柱形跨声速激波的存在稳定性,利用 deformation-curl 分解和 Rankine-Hugoniot 条件重构,唯一确定自由激波锋面并获得最优正则性。

摘要:

我们在对背景跨声速激波解不作任何进一步限制的情况下,建立了入流和出口压力受到三维扰动时柱形跨声速激波解的存在性与稳定性。受扰动跨声速激波的强度和位置完全自由,并由入流和出口压力唯一确定。所有物理量均获得最优正则性,且速度、Bernoulli量、熵和压力具有相同的正则性。该方法基于作者提出的对定常 Euler 系统的 deformation-curl 分解,用以有效解耦双曲型与椭圆型模态。然而,应用 deformation-curl 分解的关键要素之一,是找到 Rankine-Hugoniot 条件的一种分解;这种分解揭示了由一个代数方程唯一确定激波锋面的机制,同时还在激波锋面上为一阶 deformation-curl 系统给出了一个不同寻常的二阶微分边界条件。在对 curl 系统进行齐次化并引入势函数之后,激波锋面上的这一异常条件转化为在激波锋面与柱壁交线上具有齐次 Neumann 边界条件的 Poisson 方程,由此可唯一导出势函数的一个斜边界条件。

英文摘要:

We establish the existence and stability of cylindrical transonic shock solutions under three dimensional perturbations of the incoming flows and the exit pressure without any further restrictions on the background transonic shock solutions. The strength and position of the perturbed transonic shock are completely free and uniquely determined by the incoming flows and the exit pressure. The optimal regularity is obtained for all physical quantities, and the velocity, the Bernoulli's quantity, the entropy and the pressure share the same regularity. The approach is based on the deformation-curl decomposition to the steady Euler system introduced by the authors to decouple the hyperbolic and elliptic modes effectively. However, one of the key elements in application of the deformation-curl decomposition is to find a decomposition of the Rankine-Hugoniot conditions, which shows the mechanism of determining the shock front uniquely by an algebraic equation and also gives an unusual second order differential boundary conditions on the shock front for the first order deformation-curl system. After homogenizing the curl system and introducing a potential function, this unusual condition on the shock front becomes the Poisson equation with homogeneous Neumann boundary condition on the intersection of the shock front and the cylinder walls from which an oblique boundary condition for the potential function can be uniquely derived.

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