S. E. Milan, M. K. Mooney, G. E. Bower, G. Kennedy, B. J. Anderson, S. K. Vines, M. R. Hairston
{"title":"北行星际磁场日侧场向电流重联与粘性控制","authors":"S. E. Milan, M. K. Mooney, G. E. Bower, G. Kennedy, B. J. Anderson, S. K. Vines, M. R. Hairston","doi":"10.1029/2025JA034547","DOIUrl":null,"url":null,"abstract":"<p>We study the morphology and magnitude of dayside field-aligned currents (FACs) for northward interplanetary magnetic field (IMF) using observations from the Active Magnetosphere and Planetary Electrodynamics Response Experiment (AMPERE). For near-zero IMF clock angles the FACs form a quadrupolar pattern centered at local noon, which is associated with the reverse convection cells driven by lobe reconnection. The poleward pair of FACs, known as the northward-<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>B</mi>\n <mi>Z</mi>\n </msub>\n </mrow>\n <annotation> ${B}_{Z}$</annotation>\n </semantics></math> or NBZ FAC system, comprises upward and downward FAC pre- and post-noon; and the equatorward pair have the opposite polarity. The magnitude of the NBZ FACs is modulated by dipole tilt and phase of the solar cycle, the former controlling the solar zenith angle in the vicinity of the FACs, and the latter controlling the solar radio flux at 10.7 cm (F10.7), both of which contribute to the conductance of the ionosphere. The NBZ FACs are also modulated by the magnitude of the IMF (or the Z-component of the IMF for near-zero clock angle), which we presume controls the lobe reconnection rate. The NBZ FACs do not respond to the X-component of the IMF, solar wind speed, nor solar wind density, so we presume that these do not affect the lobe reconnection rate. High solar wind speed leads to the appearance of region 1 and 2 FACs at auroral latitudes, which we suggest are associated with a viscous interaction between the solar wind and the magnetosphere.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":"130 10","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2025-10-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2025JA034547","citationCount":"0","resultStr":"{\"title\":\"Reconnection and Viscous Control of Dayside Field-Aligned Currents for Northward Interplanetary Magnetic Field\",\"authors\":\"S. E. Milan, M. K. Mooney, G. E. Bower, G. Kennedy, B. J. Anderson, S. K. Vines, M. R. Hairston\",\"doi\":\"10.1029/2025JA034547\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>We study the morphology and magnitude of dayside field-aligned currents (FACs) for northward interplanetary magnetic field (IMF) using observations from the Active Magnetosphere and Planetary Electrodynamics Response Experiment (AMPERE). For near-zero IMF clock angles the FACs form a quadrupolar pattern centered at local noon, which is associated with the reverse convection cells driven by lobe reconnection. The poleward pair of FACs, known as the northward-<span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>B</mi>\\n <mi>Z</mi>\\n </msub>\\n </mrow>\\n <annotation> ${B}_{Z}$</annotation>\\n </semantics></math> or NBZ FAC system, comprises upward and downward FAC pre- and post-noon; and the equatorward pair have the opposite polarity. The magnitude of the NBZ FACs is modulated by dipole tilt and phase of the solar cycle, the former controlling the solar zenith angle in the vicinity of the FACs, and the latter controlling the solar radio flux at 10.7 cm (F10.7), both of which contribute to the conductance of the ionosphere. The NBZ FACs are also modulated by the magnitude of the IMF (or the Z-component of the IMF for near-zero clock angle), which we presume controls the lobe reconnection rate. The NBZ FACs do not respond to the X-component of the IMF, solar wind speed, nor solar wind density, so we presume that these do not affect the lobe reconnection rate. High solar wind speed leads to the appearance of region 1 and 2 FACs at auroral latitudes, which we suggest are associated with a viscous interaction between the solar wind and the magnetosphere.</p>\",\"PeriodicalId\":15894,\"journal\":{\"name\":\"Journal of Geophysical Research: Space Physics\",\"volume\":\"130 10\",\"pages\":\"\"},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2025-10-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2025JA034547\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Geophysical Research: Space Physics\",\"FirstCategoryId\":\"89\",\"ListUrlMain\":\"https://agupubs.onlinelibrary.wiley.com/doi/10.1029/2025JA034547\",\"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://agupubs.onlinelibrary.wiley.com/doi/10.1029/2025JA034547","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
我们利用主动磁层和行星电动力学响应实验(AMPERE)的观测资料,研究了北行星际磁场(IMF)的日侧场向电流(FACs)的形态和大小。对于接近零的IMF时钟角,fac形成以当地正午为中心的四极图案,这与由叶重连驱动的反向对流细胞有关。极向的FAC对,称为北- B - Z ${B}_{Z}$或NBZ FAC系统,包括午前和午后向上和向下的FAC;而赤道方向的对则具有相反的极性。偶极子倾斜和太阳周期相位对北纬z区电离层的大小有调节作用,偶极子倾斜控制着北纬z区附近的太阳天顶角,而太阳周期相位控制着太阳射电通量在10.7 cm (F10.7)处,两者对电离层的电导都有影响。NBZ fac也由IMF的幅度(或接近零时钟角的IMF的z分量)调制,我们假设它控制着瓣重连接率。NBZ fac不响应IMF的x分量、太阳风速度和太阳风密度,因此我们假设这些不影响叶重联率。高太阳风速度导致了极光纬度1区和2区fas的出现,我们认为这与太阳风和磁层之间的粘性相互作用有关。
Reconnection and Viscous Control of Dayside Field-Aligned Currents for Northward Interplanetary Magnetic Field
We study the morphology and magnitude of dayside field-aligned currents (FACs) for northward interplanetary magnetic field (IMF) using observations from the Active Magnetosphere and Planetary Electrodynamics Response Experiment (AMPERE). For near-zero IMF clock angles the FACs form a quadrupolar pattern centered at local noon, which is associated with the reverse convection cells driven by lobe reconnection. The poleward pair of FACs, known as the northward- or NBZ FAC system, comprises upward and downward FAC pre- and post-noon; and the equatorward pair have the opposite polarity. The magnitude of the NBZ FACs is modulated by dipole tilt and phase of the solar cycle, the former controlling the solar zenith angle in the vicinity of the FACs, and the latter controlling the solar radio flux at 10.7 cm (F10.7), both of which contribute to the conductance of the ionosphere. The NBZ FACs are also modulated by the magnitude of the IMF (or the Z-component of the IMF for near-zero clock angle), which we presume controls the lobe reconnection rate. The NBZ FACs do not respond to the X-component of the IMF, solar wind speed, nor solar wind density, so we presume that these do not affect the lobe reconnection rate. High solar wind speed leads to the appearance of region 1 and 2 FACs at auroral latitudes, which we suggest are associated with a viscous interaction between the solar wind and the magnetosphere.