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On the Limit as the Density Ratio Tends to Zero for Two Perfect Incompressible Fluids Separated by a Surface of Discontinuity

机译:关于由不连续面分离的两种完全不可压缩流体的密度比趋于零的极限

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摘要

We study the asymptotic limit as the density ratio ρ−/ρ+ → 0, where ρ+ and ρ− are the densities of two perfect incompressible 2-D/3-D fluids, separated by a surface of discontinuity along which the pressure jump is proportional to the mean curvature of the moving surface. Mathematically, the fluid motion is governed by the two-phase incompressible Euler equations with vortex sheet data. By rescaling, we assume the density ρ+ of the inner fluid is fixed, while the density ρ− of the outer fluid is set to ε. We prove that solutions of the free-boundary Euler equations in vacuum are obtained in the limit as ε → 0.
机译:我们以密度比Ï ˆˆ /Ï + †0来研究渐近极限,其中Ï + 和Ï ˆ> 是两种完美的不可压缩的2-D / 3-D流体的密度,它们被不连续的表面隔开,沿该表面的压力跃变与移动表面的平均曲率成比例。在数学上,流体运动由带有涡旋数据的两相不可压缩的欧拉方程控制。通过重新缩放,我们假定内部流体的密度Ï + 是固定的,而外部流体的密度Ï âˆ 设置为µ。我们证明在自由中的自由边界Euler方程的解在极限中获得为μ0。

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  • 来源
    《Communications in Partial Differential Equations》 |2010年第5期|p.817-845|共29页
  • 作者单位

    Department of Mathematics, National Central University, Jhongli City, Taiwan;

    CANPDE, Maxwell Institute for Mathematical Sciences and Department of Mathematics, Heriot-Watt University, Edinburgh, UK;

    Department of Mathematics, University of California a;

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