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Unified theory of damping of linear surface Alfven waves in inhomogeeeous incompressible plasmas

机译:非均匀不可压缩等离子体中线性表面Alfven波阻尼的统一理论

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摘要

The viscous damping of.surface Alfven waves in a non-uniform plasma is. studied in the context of linear and incompressible MHD. It is shown that damping due to resonant absorption and damping on a true discontinuity are two limiting cases of the continuous variation of the damping rate with respect to the dimensionless number Rg = AA2Re,. where A is the relative variation of the local Alfven velocity, A is the ratio of the thickness of the inhomogeneous layer to the wavelength, and Re is the viscous Reynolds number. The analysis i.s restricted to waves with wavelengths that are long in comparison with the extent of the non-uniform layer (A 1), and to Reynolds numbers that are sufficiently large that the waves are only slightly damped during one wave period. The dispersion relation is obtained and first investigated analytically for the limiting cases of very small (Rg 1) and very large (Rg 1) values of Rg. For very small values of Rg, the damping rate agrees with that found for a true discontinuity, while for very large values of Rg, it .agrees with the damping rate due to resonant absorption. The dispersion relation is subsequently studied numerically over a wide range of values of Rg, revealing a continuous but nonmonotonic variation of the damping rate with respect to Rg.
机译:非均匀等离子体中表面Alfven波的粘性阻尼。在线性和不可压缩MHD的背景下进行了研究。结果表明,由于共振吸收引起的阻尼和真正不连续的阻尼是阻尼率相对于无量纲数Rg = AA2Re,连续变化的两种极限情况。其中A是局部Alfven速度的相对变化,A是不均匀层的厚度与波长的比率,Re是粘性雷诺数。该分析仅限于与非均匀层的范围相比波长较长的波(A 1),以及雷诺数足够大以至于在一个波周期内仅略微衰减波。获得色散关系,并首先对Rg非常小(Rg 1)和非常大(Rg 1)的极限情况进行分析研究。对于非常小的Rg值,阻尼率与真正不连续的阻尼率一致,而对于非常大的Rg值,它与共振吸收引起的阻尼率一致。随后,在较大的Rg值范围内对色散关系进行了数值研究,揭示了阻尼率相对于Rg连续但非单调变化。

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