L. Rusaitis, M. El-Alaoui, R. J. Walker, G. Lapenta, D. Schriver
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The primary source of particles to the inner magnetosphere is bursty bulk flows (BBFs) that originate from a complex pattern of reconnection in the near-Earth magnetotail at <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>x</mi>\n <mtext>GSM</mtext>\n </msub>\n <mo>=</mo>\n <mo>−</mo>\n <mn>18</mn>\n <msub>\n <mi>R</mi>\n <mi>E</mi>\n </msub>\n </mrow>\n <annotation> ${x}_{\\text{GSM}}=-18{R}_{\\mathrm{E}}$</annotation>\n </semantics></math> to <span></span><math>\n <semantics>\n <mrow>\n <mo>−</mo>\n <mn>30</mn>\n <msub>\n <mi>R</mi>\n <mi>E</mi>\n </msub>\n </mrow>\n <annotation> ${-}30{R}_{\\mathrm{E}}$</annotation>\n </semantics></math>. Most ion acceleration occurs in this region, gaining from 10 to 50 keV as they traverse the sites of active reconnection. Electrons jet away from the reconnection region much faster than the ions, setting up an ambipolar electric field allowing the ions to catch up after approximately 10 ion inertial lengths. The initial energy flux in the BBFs is mainly kinetic energy flux from the ions, but as they move earthward, the energy flux changes to enthalpy flux at the ring current. The power delivered from the tail reconnection in the simulation to the inner magnetosphere is <span></span><math>\n <semantics>\n <mrow>\n <mo>></mo>\n <mn>2</mn>\n <mo>×</mo>\n <mn>1</mn>\n <msup>\n <mn>0</mn>\n <mn>11</mn>\n </msup>\n </mrow>\n <annotation> ${ >} 2\\times 1{0}^{11}$</annotation>\n </semantics></math> W, which is consistent with observations.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":null,"pages":null},"PeriodicalIF":2.6000,"publicationDate":"2024-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Multi-Scale Particle-In-Cell Simulation of Plasma Dynamics From Magnetotail Reconnection to the Inner Magnetosphere\",\"authors\":\"L. Rusaitis, M. El-Alaoui, R. J. Walker, G. Lapenta, D. Schriver\",\"doi\":\"10.1029/2024JA032821\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>During magnetospheric substorms, plasma from magnetic reconnection in the magnetotail is thought to reach the inner magnetosphere and form a partial ring current. We simulate this process using a fully kinetic 3D particle-in-cell (PIC) numerical code along with a global magnetohydrodynamics (MHD) model. The PIC simulation extends from the solar wind outside the bow shock to beyond the reconnection region in the tail, while the MHD code extends much further and is run for nominal solar wind parameters and a southward interplanetary magnetic field. By the end of the PIC calculation, ions and electrons from the tail reconnection reach the inner magnetosphere and form a partial ring current and diamagnetic current. The primary source of particles to the inner magnetosphere is bursty bulk flows (BBFs) that originate from a complex pattern of reconnection in the near-Earth magnetotail at <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>x</mi>\\n <mtext>GSM</mtext>\\n </msub>\\n <mo>=</mo>\\n <mo>−</mo>\\n <mn>18</mn>\\n <msub>\\n <mi>R</mi>\\n <mi>E</mi>\\n </msub>\\n </mrow>\\n <annotation> ${x}_{\\\\text{GSM}}=-18{R}_{\\\\mathrm{E}}$</annotation>\\n </semantics></math> to <span></span><math>\\n <semantics>\\n <mrow>\\n <mo>−</mo>\\n <mn>30</mn>\\n <msub>\\n <mi>R</mi>\\n <mi>E</mi>\\n </msub>\\n </mrow>\\n <annotation> ${-}30{R}_{\\\\mathrm{E}}$</annotation>\\n </semantics></math>. Most ion acceleration occurs in this region, gaining from 10 to 50 keV as they traverse the sites of active reconnection. Electrons jet away from the reconnection region much faster than the ions, setting up an ambipolar electric field allowing the ions to catch up after approximately 10 ion inertial lengths. The initial energy flux in the BBFs is mainly kinetic energy flux from the ions, but as they move earthward, the energy flux changes to enthalpy flux at the ring current. The power delivered from the tail reconnection in the simulation to the inner magnetosphere is <span></span><math>\\n <semantics>\\n <mrow>\\n <mo>></mo>\\n <mn>2</mn>\\n <mo>×</mo>\\n <mn>1</mn>\\n <msup>\\n <mn>0</mn>\\n <mn>11</mn>\\n </msup>\\n </mrow>\\n <annotation> ${ >} 2\\\\times 1{0}^{11}$</annotation>\\n </semantics></math> W, which is consistent with observations.</p>\",\"PeriodicalId\":15894,\"journal\":{\"name\":\"Journal of Geophysical Research: Space Physics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2024-09-23\",\"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/10.1029/2024JA032821\",\"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/10.1029/2024JA032821","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
在磁层亚暴期间,磁尾磁重连接产生的等离子体被认为会到达内磁层并形成部分环流。我们使用全动力学三维粒子在胞(PIC)数值代码和全局磁流体力学(MHD)模型模拟了这一过程。PIC 模拟从弓形冲击外的太阳风一直延伸到尾部重连接区域之外,而 MHD 代码则延伸得更远,并且是在标称太阳风参数和行星际磁场向南的情况下运行的。在 PIC 计算结束时,来自尾部重联的离子和电子到达内部磁层,形成部分环流和二磁流。内磁层的主要粒子源是爆发性大体流(BBFs),它源自近地磁尾中 x GSM = - 18 R E ${x}_{text{GSM}}=-18{R}_\{mathrm{E}}$ 到 - 30 R E ${-}30{R}_\{mathrm{E}}$ 的复杂重联模式。大部分离子加速都发生在这一区域,当它们穿过活跃的再连接点时,会获得 10 到 50 keV 的加速度。电子以比离子更快的速度喷射离开重联区域,从而建立起一个极性电场,使离子能够在大约 10 个离子惯性长度之后赶上。BBF 中的初始能量通量主要是来自离子的动能通量,但当它们向地球移动时,能量通量会转变为环流的焓通量。模拟中从尾部再连接传递到内部磁层的功率为 > 2 × 1 0 11 ${ >} 2\times 1{0}^{11}$ W,这与观测结果一致。
A Multi-Scale Particle-In-Cell Simulation of Plasma Dynamics From Magnetotail Reconnection to the Inner Magnetosphere
During magnetospheric substorms, plasma from magnetic reconnection in the magnetotail is thought to reach the inner magnetosphere and form a partial ring current. We simulate this process using a fully kinetic 3D particle-in-cell (PIC) numerical code along with a global magnetohydrodynamics (MHD) model. The PIC simulation extends from the solar wind outside the bow shock to beyond the reconnection region in the tail, while the MHD code extends much further and is run for nominal solar wind parameters and a southward interplanetary magnetic field. By the end of the PIC calculation, ions and electrons from the tail reconnection reach the inner magnetosphere and form a partial ring current and diamagnetic current. The primary source of particles to the inner magnetosphere is bursty bulk flows (BBFs) that originate from a complex pattern of reconnection in the near-Earth magnetotail at to . Most ion acceleration occurs in this region, gaining from 10 to 50 keV as they traverse the sites of active reconnection. Electrons jet away from the reconnection region much faster than the ions, setting up an ambipolar electric field allowing the ions to catch up after approximately 10 ion inertial lengths. The initial energy flux in the BBFs is mainly kinetic energy flux from the ions, but as they move earthward, the energy flux changes to enthalpy flux at the ring current. The power delivered from the tail reconnection in the simulation to the inner magnetosphere is W, which is consistent with observations.