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arXiv 0905.3937math.AP
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粘性系数为零的可压缩磁流体动力学方程的不可压缩极限

Incompressible limit of the compressible magnetohydrodynamic equations with vanishing viscosity coefficients

Song Jiang, Qiangchang Ju, Fucai Li

摘要:

本文研究了粘性系数为零的可压缩磁流体动力学方程组的不可压极限,其初值为全空间$\mathbb{R}^d$ $ (d=2$或3).严格地证明了,当马赫数、剪切粘性系数和磁扩散系数同时趋于零时,只要理想不可压磁流体力学方程组的强解存在,可压缩磁流体力学方程组的弱解收敛于理想不可压磁流体力学方程组的强解.

英文摘要:

This paper is concerned with the incompressible limit of the compressible magnetohydrodynamic equations with vanishing viscosity coefficients and general initial data in the whole space $\mathbb{R}^d$ $ (d=2$ or 3). It is rigorously showed that, as the Mach number, the shear viscosity coefficient and the magnetic diffusion coefficient simultaneously go to zero, the weak solution of the compressible magnetohydrodynamic equations converges to the strong solution of the ideal incompressible magnetohydrodynamic equations as long as the latter exists.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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