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Barotropic, baroclinic, and inertial instabilities of the easterly Gaussian jet on the equatorial β-plane in rotating shallow water model

机译:旋转浅水模型中赤道β平面上东风高斯射流的正压,斜压和惯性不稳定性

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摘要

A detailed linear stability analysis of an easterly barotropic Gaussian jet centered at the equator is performed in the long-wave sector in the framework of one- and twolayer shallow-water models on the equatorial β-plane. It is shown that the dominant instability of the jet is due to phase-locking and resonance between Yanai waves, although the standard barotropic and baroclinic instabilities due to the resonance between Rossby waves are also present. In the one-layer case, this dominant instability has non-zero growth rate at zero wavenumber for high enough Rossby and low enough Burger numbers, thus reproducing the classical symmetric inertial instability. Yet its asymmetric counterpart has the highest growth rate. In the two-layer case, the dominant instability may be barotropic or baroclinic, the latter being stronger, with the maximum of the growth rate shifting towards smaller downstream wavenumbers as Rossby number increases at fixed Burger number, and given thickness and density ratios. At large enough Rossby numbers this instability has a non-zero growth rate limit at zero wavenumber, giving the baroclinic symmetric inertial instability. Again, the maximal growth rate is achieved at small but non-zero wavenumbers, corresponding to the asymmetric inertial instability. At high enough Rossby number and low enough Burger number not only the baroclinic, but also the barotropic symmetric instability appears, as well as higher meridional modes of the baroclinic symmetric instability. Still, all of them are dominated by their asymmetric counterparts. Direct numerical simulations of the saturation of the leading instabilities are performed, showing that the barotropic species of the instability saturates by forming a double vortex street subject to nonlinear oscillations, while the baroclinic, the most vigorous one, saturates by producing strong vertical shears and related dissipation and mixing.
机译:在赤道β平面上的一层和两层浅水模型的框架内,在长波区域内对以赤道为中心的东风正压高斯射流进​​行了详细的线性稳定性分析。结果表明,喷流的主要不稳定性是由柳井波之间的锁相和共振引起的,尽管由于罗斯比波之间的共振也存在标准的正压和斜压不稳定性。在单层情况下,对于足够高的Rossby和足够低的Burger数,这种主导性不稳定性在零波数下具有非零的增长率,从而再现了经典的对称惯性不稳定性。然而,其不对称同行的增长率最高。在两层情况下,主要的不稳定性可能是正压或斜压,后者更强,随着罗斯比数在固定的汉堡数下增加,并且给定厚度和密度比,增长率的最大值会向较小的下游波数转移。在足够大的Rossby数下,这种不稳定性在零波数下具有非零的增长率限制,从而产生了斜压对称惯性不稳定性。同样,在较小但非零的波数下实现了最大增长率,这对应于非对称惯性不稳定性。在足够高的Rossby数和足够低的Burger数下,不仅出现了斜压,而且出现了正压对称不稳定性,以及更高的子午线对称不稳定性的子午模式。尽管如此,所有这些都由不对称的对等体主导。对前导不稳定性的饱和度进行了直接数值模拟,结果表明,不稳定性的正压物质通过形成一条受非线性振荡影响的双涡流街而饱和,而最强的斜压因产生强烈的垂直切变而饱和。耗散和混合。

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