Two current systems in the preliminary phase of sudden commencements in the magnetosphere
Abstract The preliminary impulse of the sudden commencement is simply explained by the generation of the compressional wave due to sudden compression of the dayside magnetopause and mode conversion from the compressional wave to the Alfvén wave in the magnetosphere. However, this simple model cannot...
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| Format: | Article |
| Language: | English |
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SpringerOpen
2022-04-01
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| Series: | Earth, Planets and Space |
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| Online Access: | https://doi.org/10.1186/s40623-022-01624-3 |
| _version_ | 1818012325036163072 |
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| author | Shigeru Fujita Takashi Tanaka |
| author_facet | Shigeru Fujita Takashi Tanaka |
| author_sort | Shigeru Fujita |
| collection | DOAJ |
| description | Abstract The preliminary impulse of the sudden commencement is simply explained by the generation of the compressional wave due to sudden compression of the dayside magnetopause and mode conversion from the compressional wave to the Alfvén wave in the magnetosphere. However, this simple model cannot explain a time delay of the peak displacement and longer duration time in the higher latitudes in the pre-noon and post-noon sectors of the polar region. Based on the global magnetohydrodynamic simulation of the magnetosphere–ionosphere system reveals that this peculiar behavior of the geomagnetic variation of the preliminary impulse is associated with temporal deformation of the ionospheric field-aligned current distribution of the preliminary impulse into a crescent shape; its lower-latitude edge extends toward the anti-sunward direction, and its higher-latitude edge almost stays on the same longitude near noon. Numerical simulations revealed that the deformation of the field-aligned current distribution is derived from different behaviors of the two current systems of the preliminary impulse. The first current system consists of the field-aligned current connected to the field-aligned current of the preliminary impulse in the lower latitude side of the ionosphere, the cross-magnetopause current, and the magnetosheath current (type L current system). The cross-magnetopause current is the inertia current generated in the acceleration front of the solar wind due to the sudden compression of the magnetosheath. Thus, the longitudinal speed of the type L current system in the ionosphere is the solar wind speed in the magnetosheath projected into the ionosphere. In contrast, the current system of the preliminary impulse connected to the field-aligned current of the preliminary impulse at higher latitude (type H current system) consists of the upward/downward field-aligned current in the pre-noon/post-noon sector, respectively, and dawn-to-dusk field-perpendicular current along the dayside magnetopause. The dawn-to-dusk field-perpendicular current moves to the higher latitudes in the outer magnetosphere over time. The field-aligned current of the type H current system is converted from the field-perpendicular current due to convergence of the return field-perpendicular current heading toward the sunward direction in the outer magnetosphere; the return field-perpendicular current is the inertia current driven by the magnetospheric plasma flow associated with compression of the magnetopause behind the front region of the accelerated solar wind. The acceleration front spreads concentrically from the subsolar point. Consequently, as the return field-perpendicular current is converted to the field-aligned current of the type H current system, it does not move much in the longitudinal direction over time because the dawn-to-dusk field-perpendicular current of the type H current system moves to the higher latitudes. Therefore, the high-latitude edge of the current distribution of the preliminary impulse in the ionosphere moves only slightly. Finally, we clarified that the conversion between field-perpendicular current and field-aligned current of the type L current system mainly occurs in the region where the Alfvén speed starts to increase toward the Earth. A region with a steep gradient of the Alfvén speed like the plasmapause is not always necessary for conversion from the field-perpendicular current to the field-aligned current. We also suggest the possible field-aligned structure of the standing Alfvén wave that may occur in the preliminary impulse phase. Graphical Abstract |
| first_indexed | 2024-04-14T06:18:52Z |
| format | Article |
| id | doaj.art-77214f92248a403e88d17fcdf557d1bd |
| institution | Directory Open Access Journal |
| issn | 1880-5981 |
| language | English |
| last_indexed | 2024-04-14T06:18:52Z |
| publishDate | 2022-04-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | Earth, Planets and Space |
| spelling | doaj.art-77214f92248a403e88d17fcdf557d1bd2022-12-22T02:08:06ZengSpringerOpenEarth, Planets and Space1880-59812022-04-0174111710.1186/s40623-022-01624-3Two current systems in the preliminary phase of sudden commencements in the magnetosphereShigeru Fujita0Takashi Tanaka1Joint Support-Center for Data Science Research, Research Organization of Information and Systems (ROIS)International Center for Space Weather Science and Education, Kyushu UniversityAbstract The preliminary impulse of the sudden commencement is simply explained by the generation of the compressional wave due to sudden compression of the dayside magnetopause and mode conversion from the compressional wave to the Alfvén wave in the magnetosphere. However, this simple model cannot explain a time delay of the peak displacement and longer duration time in the higher latitudes in the pre-noon and post-noon sectors of the polar region. Based on the global magnetohydrodynamic simulation of the magnetosphere–ionosphere system reveals that this peculiar behavior of the geomagnetic variation of the preliminary impulse is associated with temporal deformation of the ionospheric field-aligned current distribution of the preliminary impulse into a crescent shape; its lower-latitude edge extends toward the anti-sunward direction, and its higher-latitude edge almost stays on the same longitude near noon. Numerical simulations revealed that the deformation of the field-aligned current distribution is derived from different behaviors of the two current systems of the preliminary impulse. The first current system consists of the field-aligned current connected to the field-aligned current of the preliminary impulse in the lower latitude side of the ionosphere, the cross-magnetopause current, and the magnetosheath current (type L current system). The cross-magnetopause current is the inertia current generated in the acceleration front of the solar wind due to the sudden compression of the magnetosheath. Thus, the longitudinal speed of the type L current system in the ionosphere is the solar wind speed in the magnetosheath projected into the ionosphere. In contrast, the current system of the preliminary impulse connected to the field-aligned current of the preliminary impulse at higher latitude (type H current system) consists of the upward/downward field-aligned current in the pre-noon/post-noon sector, respectively, and dawn-to-dusk field-perpendicular current along the dayside magnetopause. The dawn-to-dusk field-perpendicular current moves to the higher latitudes in the outer magnetosphere over time. The field-aligned current of the type H current system is converted from the field-perpendicular current due to convergence of the return field-perpendicular current heading toward the sunward direction in the outer magnetosphere; the return field-perpendicular current is the inertia current driven by the magnetospheric plasma flow associated with compression of the magnetopause behind the front region of the accelerated solar wind. The acceleration front spreads concentrically from the subsolar point. Consequently, as the return field-perpendicular current is converted to the field-aligned current of the type H current system, it does not move much in the longitudinal direction over time because the dawn-to-dusk field-perpendicular current of the type H current system moves to the higher latitudes. Therefore, the high-latitude edge of the current distribution of the preliminary impulse in the ionosphere moves only slightly. Finally, we clarified that the conversion between field-perpendicular current and field-aligned current of the type L current system mainly occurs in the region where the Alfvén speed starts to increase toward the Earth. A region with a steep gradient of the Alfvén speed like the plasmapause is not always necessary for conversion from the field-perpendicular current to the field-aligned current. We also suggest the possible field-aligned structure of the standing Alfvén wave that may occur in the preliminary impulse phase. Graphical Abstracthttps://doi.org/10.1186/s40623-022-01624-3Sudden commencementPreliminary impulseMagnetospheric current systemLongitudinal propagation speedComputer simulationGeneration of the field-aligned current |
| spellingShingle | Shigeru Fujita Takashi Tanaka Two current systems in the preliminary phase of sudden commencements in the magnetosphere Earth, Planets and Space Sudden commencement Preliminary impulse Magnetospheric current system Longitudinal propagation speed Computer simulation Generation of the field-aligned current |
| title | Two current systems in the preliminary phase of sudden commencements in the magnetosphere |
| title_full | Two current systems in the preliminary phase of sudden commencements in the magnetosphere |
| title_fullStr | Two current systems in the preliminary phase of sudden commencements in the magnetosphere |
| title_full_unstemmed | Two current systems in the preliminary phase of sudden commencements in the magnetosphere |
| title_short | Two current systems in the preliminary phase of sudden commencements in the magnetosphere |
| title_sort | two current systems in the preliminary phase of sudden commencements in the magnetosphere |
| topic | Sudden commencement Preliminary impulse Magnetospheric current system Longitudinal propagation speed Computer simulation Generation of the field-aligned current |
| url | https://doi.org/10.1186/s40623-022-01624-3 |
| work_keys_str_mv | AT shigerufujita twocurrentsystemsinthepreliminaryphaseofsuddencommencementsinthemagnetosphere AT takashitanaka twocurrentsystemsinthepreliminaryphaseofsuddencommencementsinthemagnetosphere |