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Multi-dimensional compressible Navier-Stokes equations with free boundary and symmetry.

机译:具有自由边界和对称性的多维可压缩Navier-Stokes方程。

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摘要

The motivation of this work has come from the fluid thermodynamics. Dynamics of a viscous polytropic gas can be described by the compressible Navier-Stokes equations of conservation of mass, momentum, and energy. We study and prove the global existence of a weak solution in a domain outside of a solid core, assuming spherical symmetry and a free boundary. The gas dynamics close to the free boundary with the surrounding vacuum is described by the stress free condition and the zero heat flux requirement. Initially, the gas is assumed to continuously fill finite volume with bounded positive density between the static core and the free boundary. The absolute temperature of the gas is assumed to be initially bounded and strictly positive.; The proof of the global existence is carried out in several important steps. The Lagrangian transformation and the symmetry assumption enable us to transform the equations into one-dimensional form with geometrical source terms over a fixed mass domain. A sequence of solutions to approximate problems is constructed by using the space discretization method. With the help of a priori energy estimates, we show their global time existence, prove their weak convergence, and show that their limit is a solution to the original problem. The key milestones in the process of obtaining energy estimates include the property of finite free boundary expansion, the dissipation of the generalized total energy, the uniform point-wise boundedness of the density and the velocity, the uniform relative point-wise boundedness of the density from below, the uniform boundedness of the temperature away from the absolute zero, and the weak form of the temperature boundedness from above. These results are accompanied by quite a few higher order energy estimates that are necessary for the compactness framework and form the base for our convergence arguments. At the end we discuss classical solutions, external forces, and other extensions of our main results.
机译:这项工作的动机来自流体的热力学。粘性多变气体的动力学可以通过守恒质量,动量和能量的可压缩Navier-Stokes方程来描述。我们研究并证明了在球心对称和自由边界的情况下,在实心之外的区域中弱解的整体存在性。通过无应力条件和零热通量要求来描述与周围真空接近自由边界的气体动力学。最初,假定气体以静态核心和自由边界之间的有限正密度连续填充有限体积。假定气体的绝对温度最初是有界的并且严格为正。全球存在的证明是通过几个重要步骤进行的。拉格朗日变换和对称假设使我们能够将方程式转换为具有固定质量域上的几何源项的一维形式。使用空间离散化方法构造了一系列近似问题的解决方案。在先验能量估计的帮助下,我们显示了它们的整体时间存在性,证明了它们的弱收敛性,并证明了它们的极限是对原始问题的解决方案。获得能量估计值的过程中的关键里程碑包括:有限自由边界扩展的性质,广义总能量的耗散,密度和速度的均匀点向有界性,密度的均匀点向有界性从下面开始,温度的有界边界远离绝对零,而从上面开始的温度有界的弱形式。这些结果伴随着相当多的高阶能量估计,这对于紧凑性框架是必需的,并为我们的收敛论证奠定了基础。最后,我们讨论了经典解决方案,外力以及主要结果的其他扩展。

著录项

  • 作者

    Kratka, Milan.;

  • 作者单位

    The University of Chicago.;

  • 授予单位 The University of Chicago.;
  • 学科 Mathematics.
  • 学位 Ph.D.
  • 年度 1998
  • 页码 127 p.
  • 总页数 127
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 数学;
  • 关键词

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