等温大气中特定的声粒波模式

Pub Date : 2023-04-28 DOI:10.15407/knit2023.02.045
A. Fedorenko, Yu. O. Klymenko, O. Cheremnykh, Y. Kryuchkov, I. Zhuk
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引用次数: 0

摘要

在本文中,我们证明了等温大气中重力声波的频谱包括四种特定的倏逝模式。这些模式是在假设其中一个量(粒子速度、密度波动或温度的水平或垂直分量)等于零的情况下,小型大气扰动的流体动力学方程组的解。四种特定模式中的三种(兰姆波、Brunt-Väisälä振荡和f模式)是众所周知的,但它们以前是作为独立解获得的。作者最近发现的倏逝γ模式使我们有可能表明,所有四种特定模式都形成了等温大气的特定模式家族。在频率和波矢量的频谱图上,有四条这些特殊模式的色散曲线,其中一个扰动量等于零。这些曲线属于声学重力波频谱的倏逝区域。它们在五点相交。结果表明,特定模式不能在交叉点处相互作用。如果特定曲线上的一个量为零,则两个扰动量之间的极化率在该曲线的任一侧都具有不同的符号。这些特性可作为AGW倏逝光谱实验研究中特定模式的指标。利用偏振关系,还分析了在地球大气层和太阳上观测这些模式的可能性。
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SPECIFIC ACOUSTIC-GRAVITY WAVE MODES IN ISOTHERMAL ATMOSPHERE
In the paper, we show that the spectrum of acoustic-gravity waves in an isothermal atmosphere includes four specific evanescent modes. These modes are the solutions of the system of hydrodynamic equations for small atmospheric disturbances under the assumption that one of the quantities (horizontal or vertical components of particle velocity, density fluctuations, or temperature) is equal to zero. Three of the four specific modes (the Lamb wave, the Brunt-Väisälä oscillation, and the f-mode) are well known, but they were previously obtained as independent solutions. The recent discovery by the authors of the evanescent γ-mode made it possible to show that all four specified modes form a certain family of special modes of the isothermal atmosphere. On the spectral diagram of the frequency and the wave vector, there are four dispersion curves of these special modes in which one of the perturbed quantities is equal to zero. These curves belong to the evanescent region of the acoustic-gravity wave spectrum. They intersect each other at five points. It is shown that the specific modes cannot interact at the intersection points. The polarization ratios between two perturbed quantities have a different sign on either side of a particular curve if one of the quantities on this curve is zero. These properties can be used as indicators of the specific modes in experimental studies of the evanescent spectrum of AGWs. By using polarization relations, the possibility of observing these modes in the Earth’s atmosphere and on the Sun is also analyzed.
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