{"title":"A Numerical Study on the Responses of Thermosphere Density to the IMF \n \n \n \n B\n y\n \n \n ${B}_{y}$\n Condition at High Latitudes","authors":"Yusha Tan, Jiuhou Lei, Zhongli Li, Xiaoli Luan, Xiankang Dou","doi":"10.1029/2025JA034113","DOIUrl":null,"url":null,"abstract":"<p>When the Interplanetary magnetic field (IMF) <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>B</mi>\n <mi>y</mi>\n </msub>\n </mrow>\n <annotation> ${B}_{y}$</annotation>\n </semantics></math> condition disturbs, the ionospheric convection pattern is tilted, subsequently altering thermospheric dynamics. While both observations and simulations have shown that the thermospheric mass density exhibits significantly different patterns under positive and negative IMF <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>B</mi>\n <mi>y</mi>\n </msub>\n </mrow>\n <annotation> ${B}_{y}$</annotation>\n </semantics></math> conditions, the underlying mechanisms driving the density variations at different altitudes are not well-established. In this study, we investigate the physical mechanisms responsible for the density variations based on the Thermosphere Ionosphere Electrodynamics General Circulation Model simulations. The model simulations show strong consistency with observations and indicate that density variations have universal time dependence. Meanwhile, the density variations driven by IMF <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>B</mi>\n <mi>y</mi>\n </msub>\n </mrow>\n <annotation> ${B}_{y}$</annotation>\n </semantics></math> disturbance exhibit different mechanisms in the lower and upper thermosphere. In particular, at around 200 km, the effect of non-local thermal variations dominates density changes, where the altitude-integrated effect of neutral temperature changes at lower altitudes primarily drives mass density variations at higher altitudes. At around 400 km, the composition effect associated with local vertical wind becomes the dominant driver in changing the mass density.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":"130 8","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2025-08-25","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://agupubs.onlinelibrary.wiley.com/doi/10.1029/2025JA034113","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
Abstract
When the Interplanetary magnetic field (IMF) condition disturbs, the ionospheric convection pattern is tilted, subsequently altering thermospheric dynamics. While both observations and simulations have shown that the thermospheric mass density exhibits significantly different patterns under positive and negative IMF conditions, the underlying mechanisms driving the density variations at different altitudes are not well-established. In this study, we investigate the physical mechanisms responsible for the density variations based on the Thermosphere Ionosphere Electrodynamics General Circulation Model simulations. The model simulations show strong consistency with observations and indicate that density variations have universal time dependence. Meanwhile, the density variations driven by IMF disturbance exhibit different mechanisms in the lower and upper thermosphere. In particular, at around 200 km, the effect of non-local thermal variations dominates density changes, where the altitude-integrated effect of neutral temperature changes at lower altitudes primarily drives mass density variations at higher altitudes. At around 400 km, the composition effect associated with local vertical wind becomes the dominant driver in changing the mass density.
当行星际磁场(IMF) B y ${B}_{y}$条件扰动时,电离层对流模式发生倾斜,从而改变热层动力学。虽然观测和模拟都表明,在正、负IMF B y ${B}_{y}$条件下,热层质量密度表现出明显不同的模式,但不同高度下驱动密度变化的潜在机制尚未确定。本文在热层电离层电动力学环流模式模拟的基础上,探讨了密度变化的物理机制。模式模拟结果与观测结果高度一致,表明密度变化具有普遍的时间依赖性。同时,由IMF B y ${B}_{y}$扰动驱动的密度变化在上下热层表现出不同的机制。特别是在200公里左右,非局地热变化的影响主导了密度变化,其中低海拔中性温度变化的高度综合效应主要驱动高海拔的质量密度变化。在400 km左右,与局地垂直风相关的成分效应成为改变质量密度的主要驱动因素。