Some Exact Blowup Solutions to the Pressureless Euler Equations in R^N

preprint2009arXivOpen access

Abstract

The pressureless Euler equations can be used as simple models of cosmology or plasma physics. In this paper, we construct the exact solutions in non-radial symmetry to the pressureless Euler equations in RN:R^{N}:% [c]{c}% ρ(t,\vec{x})=\frac{f(\frac{1}{a(t)^{s}}\underset{i=1}{\overset {N}{\sum}}x_{i}^{s})}{a(t)^{N}}\text{,}\vec{u}(t,\vec{x}% )=\frac{\overset{\cdot}{a}(t)}{a(t)}\vec{x}, a(t)=a_{1}+a_{2}t. \label{eq234}% where the arbitrary function f≥0f\geq0 and f∈C1;f\in C^{1}; s≥1s\geq1, a1>0a_{1}>0 and a2a_{2} are constants..\newline In particular, for a2<0a_{2}<0, the solutions blow up on the finite time T=−a1/a2T=-a_{1}/a_{2}. Moreover, the functions (\ref{eq234}) are also the solutions to the pressureless Navier-Stokes equations.

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