{"title":"扰动条件下高纬度离子-中性耦合时间尺度的数值研究","authors":"Yusha Tan, Jiuhou Lei, Tong Dang, Wenbin Wang, Binzheng Zhang, Xiaoli Luan, Xiankang Dou","doi":"10.1029/2024JA032497","DOIUrl":null,"url":null,"abstract":"<p>When solar wind and interplanetary magnetic field (IMF) disturb, thermospheric winds change accordingly. Among the momentum forces driving high-latitude thermospheric winds, ion drag is supposed to greatly affect wind variations through ion-neutral coupling when abrupt and strong changes in ion drifts occur. However, due to the great inertia of thermospheric winds it needs a certain period of time for the wind changes to be prominent both in speed and direction. How long the neutral winds take to change from one steady state to another through the ion-neutral coupling process is currently still a controversial issue. In this paper, we examine the high latitudinal ion-neutral coupling time scale based on the Thermosphere Ionosphere Electrodynamics General Circulation Model simulations, which can determine whether wind variations are dominantly driven by ion drag by analyzing the relative contribution of each momentum force. It is found that the spatial variation of ion-neutral coupling time scale is primarily determined by local electron density, but also varies with neutral density and ion-neutral collision frequency. Simulations during periods of medium solar activity at ∼250 km altitude show that the ion drag-dominated region is generally located at the dayside convection inverse boundary and the coupling time scale (e-folding time) is ∼1 hr when IMF <i>B</i><sub><i>y</i></sub> is the dominant component of the IMF and changes direction. Meanwhile, the southward component of IMF <i>B</i><sub><i>z</i></sub> enlarges the ion drag-dominated region. When IMF <i>B</i><sub><i>z</i></sub> is southward with a large magnitude, ion drag-dominated region is primarily located in the nightside auroral oval with ∼2 hr coupling time scale.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":null,"pages":null},"PeriodicalIF":2.6000,"publicationDate":"2024-07-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Numerical Study of the High Latitudinal Ion-Neutral Coupling Time Scale Under Disturbed Conditions\",\"authors\":\"Yusha Tan, Jiuhou Lei, Tong Dang, Wenbin Wang, Binzheng Zhang, Xiaoli Luan, Xiankang Dou\",\"doi\":\"10.1029/2024JA032497\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>When solar wind and interplanetary magnetic field (IMF) disturb, thermospheric winds change accordingly. Among the momentum forces driving high-latitude thermospheric winds, ion drag is supposed to greatly affect wind variations through ion-neutral coupling when abrupt and strong changes in ion drifts occur. However, due to the great inertia of thermospheric winds it needs a certain period of time for the wind changes to be prominent both in speed and direction. How long the neutral winds take to change from one steady state to another through the ion-neutral coupling process is currently still a controversial issue. In this paper, we examine the high latitudinal ion-neutral coupling time scale based on the Thermosphere Ionosphere Electrodynamics General Circulation Model simulations, which can determine whether wind variations are dominantly driven by ion drag by analyzing the relative contribution of each momentum force. It is found that the spatial variation of ion-neutral coupling time scale is primarily determined by local electron density, but also varies with neutral density and ion-neutral collision frequency. Simulations during periods of medium solar activity at ∼250 km altitude show that the ion drag-dominated region is generally located at the dayside convection inverse boundary and the coupling time scale (e-folding time) is ∼1 hr when IMF <i>B</i><sub><i>y</i></sub> is the dominant component of the IMF and changes direction. Meanwhile, the southward component of IMF <i>B</i><sub><i>z</i></sub> enlarges the ion drag-dominated region. When IMF <i>B</i><sub><i>z</i></sub> is southward with a large magnitude, ion drag-dominated region is primarily located in the nightside auroral oval with ∼2 hr coupling time scale.</p>\",\"PeriodicalId\":15894,\"journal\":{\"name\":\"Journal of Geophysical Research: Space Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2024-07-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Geophysical Research: Space Physics\",\"FirstCategoryId\":\"89\",\"ListUrlMain\":\"https://onlinelibrary.wiley.com/doi/10.1029/2024JA032497\",\"RegionNum\":2,\"RegionCategory\":\"地球科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ASTRONOMY & ASTROPHYSICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Geophysical Research: Space Physics","FirstCategoryId":"89","ListUrlMain":"https://onlinelibrary.wiley.com/doi/10.1029/2024JA032497","RegionNum":2,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0
摘要
当太阳风和行星际磁场(IMF)发生扰动时,热层风也会发生相应的变化。在驱动高纬度热层风的动量中,当离子漂移发生突然而强烈的变化时,离子阻力应该会通过离子-中性耦合对风的变化产生很大影响。然而,由于热层风的巨大惯性,风速和风向的变化都需要一定的时间才能显现出来。中性风通过离子-中性耦合过程从一种稳定状态转变为另一种稳定状态需要多长时间,目前仍是一个有争议的问题。本文基于热层电离层电动力学大气环流模式模拟,研究了高纬度离子-中性风耦合时间尺度,通过分析各动量的相对贡献,确定风的变化是否主要由离子阻力驱动。研究发现,离子-中性耦合时间尺度的空间变化主要由当地电子密度决定,但也随中性密度和离子-中性碰撞频率的变化而变化。在高度为 ∼250 km 的中等太阳活动期间进行的模拟显示,当 IMF By 为 IMF 的主导成分并改变方向时,离子阻力主导区域一般位于日侧对流逆边界,耦合时间尺度(e-折叠时间)为 ∼1 小时。同时,IMF Bz的南向分量扩大了离子阻力主导区域。当IMF Bz南下且幅度较大时,离子阻力主导区主要位于极光椭圆夜侧,耦合时间尺度为∼2小时。
A Numerical Study of the High Latitudinal Ion-Neutral Coupling Time Scale Under Disturbed Conditions
When solar wind and interplanetary magnetic field (IMF) disturb, thermospheric winds change accordingly. Among the momentum forces driving high-latitude thermospheric winds, ion drag is supposed to greatly affect wind variations through ion-neutral coupling when abrupt and strong changes in ion drifts occur. However, due to the great inertia of thermospheric winds it needs a certain period of time for the wind changes to be prominent both in speed and direction. How long the neutral winds take to change from one steady state to another through the ion-neutral coupling process is currently still a controversial issue. In this paper, we examine the high latitudinal ion-neutral coupling time scale based on the Thermosphere Ionosphere Electrodynamics General Circulation Model simulations, which can determine whether wind variations are dominantly driven by ion drag by analyzing the relative contribution of each momentum force. It is found that the spatial variation of ion-neutral coupling time scale is primarily determined by local electron density, but also varies with neutral density and ion-neutral collision frequency. Simulations during periods of medium solar activity at ∼250 km altitude show that the ion drag-dominated region is generally located at the dayside convection inverse boundary and the coupling time scale (e-folding time) is ∼1 hr when IMF By is the dominant component of the IMF and changes direction. Meanwhile, the southward component of IMF Bz enlarges the ion drag-dominated region. When IMF Bz is southward with a large magnitude, ion drag-dominated region is primarily located in the nightside auroral oval with ∼2 hr coupling time scale.