{"title":"基于金星快车观测数据的磁子马赫数非线性效应的动态金星弓形冲击模型","authors":"Ming Wang, Qi Xu, Lianghai Xie, Lei Li, Yiteng Zhang, Jianyong Lu, Xiaojun Xu, Pingbing Zuo, Yongyong Feng, Mengsi Ruan, Tielong Zhang","doi":"10.1029/2024JA032741","DOIUrl":null,"url":null,"abstract":"<p>Utilizing the 8.5-year Venus Express observations, we investigate the effects of solar wind magnetosonic Mach number <span></span><math>\n <semantics>\n <mrow>\n <mfenced>\n <msub>\n <mi>M</mi>\n <mrow>\n <mi>M</mi>\n <mi>S</mi>\n </mrow>\n </msub>\n </mfenced>\n </mrow>\n <annotation> $\\left({M}_{MS}\\right)$</annotation>\n </semantics></math>, solar extreme ultraviolet (EUV) radiation, solar wind dynamic pressure <span></span><math>\n <semantics>\n <mrow>\n <mfenced>\n <msub>\n <mi>P</mi>\n <mi>d</mi>\n </msub>\n </mfenced>\n </mrow>\n <annotation> $\\left({P}_{d}\\right)$</annotation>\n </semantics></math> and interplanetary magnetic field (IMF) on the shape of the Venusian bow shock. Our statistical analysis yields several findings: (a) The spatial scale of the Venusian bow shock varies in a nonlinear manner with <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>M</mi>\n <mrow>\n <mi>M</mi>\n <mi>S</mi>\n </mrow>\n </msub>\n </mrow>\n <annotation> ${M}_{MS}$</annotation>\n </semantics></math> and shows a linear correlation with the EUV flux. (b) After the variance of the bow shock size caused by different <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>M</mi>\n <mrow>\n <mi>M</mi>\n <mi>S</mi>\n </mrow>\n </msub>\n </mrow>\n <annotation> ${M}_{MS}$</annotation>\n </semantics></math> and EUV are considered, the bow shock size shows no apparent correlation with the IMF intensity, IMF cone angle and solar wind dynamic pressure. (c) The angle between the IMF and the shock normal <span></span><math>\n <semantics>\n <mrow>\n <mfenced>\n <msub>\n <mi>θ</mi>\n <mrow>\n <mi>B</mi>\n <mi>n</mi>\n </mrow>\n </msub>\n </mfenced>\n </mrow>\n <annotation> $\\left({\\theta }_{Bn}\\right)$</annotation>\n </semantics></math> emerges as a significant factor shaping the bow shock's local distance. A two-parameter (<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>M</mi>\n <mrow>\n <mi>M</mi>\n <mi>S</mi>\n </mrow>\n </msub>\n </mrow>\n <annotation> ${M}_{MS}$</annotation>\n </semantics></math> and EUV) dynamic bow shock model is consequently constructed. This dynamic model not only elucidates the typical behavior of the bow shock under normal solar wind conditions but also unveils the anomalously distant bow shock location characterized by extremely low <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>M</mi>\n <mrow>\n <mi>M</mi>\n <mi>S</mi>\n </mrow>\n </msub>\n </mrow>\n <annotation> ${M}_{MS}$</annotation>\n </semantics></math>.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":null,"pages":null},"PeriodicalIF":2.6000,"publicationDate":"2024-09-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The Dynamic Venusian Bow Shock Model With the Nonlinear Effect of Magnetosonic Mach Number Based on Venus Express Observations\",\"authors\":\"Ming Wang, Qi Xu, Lianghai Xie, Lei Li, Yiteng Zhang, Jianyong Lu, Xiaojun Xu, Pingbing Zuo, Yongyong Feng, Mengsi Ruan, Tielong Zhang\",\"doi\":\"10.1029/2024JA032741\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Utilizing the 8.5-year Venus Express observations, we investigate the effects of solar wind magnetosonic Mach number <span></span><math>\\n <semantics>\\n <mrow>\\n <mfenced>\\n <msub>\\n <mi>M</mi>\\n <mrow>\\n <mi>M</mi>\\n <mi>S</mi>\\n </mrow>\\n </msub>\\n </mfenced>\\n </mrow>\\n <annotation> $\\\\left({M}_{MS}\\\\right)$</annotation>\\n </semantics></math>, solar extreme ultraviolet (EUV) radiation, solar wind dynamic pressure <span></span><math>\\n <semantics>\\n <mrow>\\n <mfenced>\\n <msub>\\n <mi>P</mi>\\n <mi>d</mi>\\n </msub>\\n </mfenced>\\n </mrow>\\n <annotation> $\\\\left({P}_{d}\\\\right)$</annotation>\\n </semantics></math> and interplanetary magnetic field (IMF) on the shape of the Venusian bow shock. Our statistical analysis yields several findings: (a) The spatial scale of the Venusian bow shock varies in a nonlinear manner with <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>M</mi>\\n <mrow>\\n <mi>M</mi>\\n <mi>S</mi>\\n </mrow>\\n </msub>\\n </mrow>\\n <annotation> ${M}_{MS}$</annotation>\\n </semantics></math> and shows a linear correlation with the EUV flux. (b) After the variance of the bow shock size caused by different <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>M</mi>\\n <mrow>\\n <mi>M</mi>\\n <mi>S</mi>\\n </mrow>\\n </msub>\\n </mrow>\\n <annotation> ${M}_{MS}$</annotation>\\n </semantics></math> and EUV are considered, the bow shock size shows no apparent correlation with the IMF intensity, IMF cone angle and solar wind dynamic pressure. (c) The angle between the IMF and the shock normal <span></span><math>\\n <semantics>\\n <mrow>\\n <mfenced>\\n <msub>\\n <mi>θ</mi>\\n <mrow>\\n <mi>B</mi>\\n <mi>n</mi>\\n </mrow>\\n </msub>\\n </mfenced>\\n </mrow>\\n <annotation> $\\\\left({\\\\theta }_{Bn}\\\\right)$</annotation>\\n </semantics></math> emerges as a significant factor shaping the bow shock's local distance. A two-parameter (<span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>M</mi>\\n <mrow>\\n <mi>M</mi>\\n <mi>S</mi>\\n </mrow>\\n </msub>\\n </mrow>\\n <annotation> ${M}_{MS}$</annotation>\\n </semantics></math> and EUV) dynamic bow shock model is consequently constructed. This dynamic model not only elucidates the typical behavior of the bow shock under normal solar wind conditions but also unveils the anomalously distant bow shock location characterized by extremely low <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>M</mi>\\n <mrow>\\n <mi>M</mi>\\n <mi>S</mi>\\n </mrow>\\n </msub>\\n </mrow>\\n <annotation> ${M}_{MS}$</annotation>\\n </semantics></math>.</p>\",\"PeriodicalId\":15894,\"journal\":{\"name\":\"Journal of Geophysical Research: Space Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2024-09-03\",\"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/10.1029/2024JA032741\",\"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/10.1029/2024JA032741","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
利用 "金星快车 "8.5年的观测数据,我们研究了太阳风磁子马赫数M M S $\left({M}_{MS}\right)$、太阳极紫外辐射(EUV)、太阳风动压P d $\left({P}_{d}\right)$和行星际磁场(IMF)对金星弓形冲击形状的影响。我们的统计分析得出了几个结论:(a)金星弓形冲击的空间尺度随 M M S ${M}_{MS}$ 呈非线性变化,并与超紫外通量呈线性相关。(b) 在考虑了不同的 M M S ${M}_{MS}$ 和 EUV 引起的弓形冲击大小差异之后,弓形冲击大小与 IMF 强度、IMF 锥角和太阳风动压没有明显的相关性。(c) IMF 与冲击法线的夹角 θ B n $\left({\theta}_{Bn}\right)$是影响弓形冲击局部距离的重要因素。因此,我们构建了一个双参数(M M S ${M}_{MS}$ 和 EUV)动态弓形冲击模型。这个动态模型不仅阐明了弓形冲击在正常太阳风条件下的典型行为,而且揭示了以极低的 M M S ${M}_{MS}$ 为特征的异常遥远的弓形冲击位置。
The Dynamic Venusian Bow Shock Model With the Nonlinear Effect of Magnetosonic Mach Number Based on Venus Express Observations
Utilizing the 8.5-year Venus Express observations, we investigate the effects of solar wind magnetosonic Mach number , solar extreme ultraviolet (EUV) radiation, solar wind dynamic pressure and interplanetary magnetic field (IMF) on the shape of the Venusian bow shock. Our statistical analysis yields several findings: (a) The spatial scale of the Venusian bow shock varies in a nonlinear manner with and shows a linear correlation with the EUV flux. (b) After the variance of the bow shock size caused by different and EUV are considered, the bow shock size shows no apparent correlation with the IMF intensity, IMF cone angle and solar wind dynamic pressure. (c) The angle between the IMF and the shock normal emerges as a significant factor shaping the bow shock's local distance. A two-parameter ( and EUV) dynamic bow shock model is consequently constructed. This dynamic model not only elucidates the typical behavior of the bow shock under normal solar wind conditions but also unveils the anomalously distant bow shock location characterized by extremely low .