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SINGULARLY PERTURBED ODES AND PROFILES FOR STATIONARY SYMMETRIC EULER AND NAVIER-STOKES SHOCKS

机译:平稳对称EULER和NAVIER-STOKS震荡的奇摄动奇异点

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摘要

We construct stationary solutions to the non-barotropic, compressible Euler and Navier-Stokes equations in several space dimensions with spherical or cylindrical symmetry. The equation of state is assumed to satisfy standard monotonicity and convexity assumptions. For given Dirichlet data on a sphere or a cylinder we first construct smooth and radially symmetric solutions to the Euler equations in an exterior domain. On the other hand, stationary smooth solutions in an interior domain necessarily become sonic and cannot be continued beyond a critical inner radius. We then use these solutions to construct entropy-satisfying shocks for the Euler equations in the region between two concentric spheres (or cylinders).Next we construct smooth solutions w~e to the Navier-Stokes system converging to the previously constructed Euler shocks in the small viscosity limit ε→ 0. The viscous solutions are obtained by a new technique for constructing solutions to a class of two-point boundary problems with a fast transition region. The construction is explicit in the sense that it produces high order expansions in powers of e for w~e, and the coefficients in the expansion satisfy simple, explicit ODEs, which are linear except in the case of the leading term. The solutions to the Euler equations described above provide the slowly varying contribution to the leading term in the expansion.The approach developed here is applicable to a variety of singular perturbation problems, including the construction of heteroclinic orbits with fast transitions. For example, a variant of our method is used in [W] to give a new construction of detonation profiles for the reactive Navier-Stokes equations.
机译:我们构造具有球形或圆柱形对称性的,在几个空间维度上的非正压,可压缩的Euler和Navier-Stokes方程的平稳解。假定状态方程满足标准单调性和凸性假设。对于球体或圆柱体上给定的Dirichlet数据,我们首先在外部域中构造Euler方程的光滑且径向对称的解。另一方面,内部区域中的平稳平稳解必定会成为声音,并且无法持续超出临界内半径。然后,我们使用这些解为两个同心球(或圆柱)之间的区域的Euler方程构造满足熵的激波。接下来,我们为Navier-Stokes系统构造光滑解,并与之前构造的Euler激波收敛。小粘度极限ε→0。粘性溶液是通过一种新技术获得的,该新技术用于构造一类具有快速过渡区域的两点边界问题的溶液。这种构造是显式的,因为它会产生e的幂幂对w〜e的高阶展开,并且展开中的系数满足简单,明确的ODE的要求,除了前导项外,它们都是线性的。上面描述的Euler方程的解为扩展中的主导项提供了缓慢变化的贡献。此处开发的方法适用于各种奇异摄动问题,包括具有快速过渡的异斜轨道的构造。例如,在[W]中使用了我们方法的一种变体,为反应性Navier-Stokes方程提供了新的爆震剖面构造。

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  • 来源
    《Discrete and continuous dynamical systems》 |2010年第1期|p.133-169|共37页
  • 作者单位

    Department of Mathematics, Penn State University University Park, State College, PA 16802, USA;

    Department of Mathematics, Penn State University University Park, State College, PA 16802, USA;

    Department of Mathematics, Univ. of North Carolina Chapel Hill, NC 27599, USA;

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