Magnetospheric Physics in China

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Magnetospheric Physics in China SPACE SCIENCE ACTIVITIES IN CHINA Magnetospheric Physics in China CAO Jinbin, YANG Junying (Space Science Institute, School of space and environment, Beihang University, Beijing 100091) National Report 2016 Abstract In the past two years, many progresses were made in magnetospheric physics by using the data of Double Star Program, Cluster, THEMIS, RBSP, Swarm, MMS, ARTEMIS, MESSENGER missions etc., or by computer simulations. This paper briefly reviews these works based on papers selected from the 227 publications from Janu- ary 2016 to December 2017. The subjects cover almost sub-branches of magnetospheric physics, including geo- magnetic storm, magnetospheric substorm, magnetic reconnection, Solar wind-magnetosphere-ionosphere interac- 2018 tion, radiation belt, plasmasphere, outer magnetosphere, magnetotail, geomagnetic field, auroras and currents. Key words Magnetospheric, Geomagnetic storms, Magnetic reconnection E-mail: [email protected] 1. Geomagnetic Storms planning, and design of low-latitude electric power networks. Geomagnetic Sudden Commencements (SCs), charac- He, F., et al., [2] present multi satellite observations terized by a rapid enhancement in the rate of change of of the evolution of Subauroral Polarization Streams the geomagnetic field perturbation (dB/dt), are consid- (SAPS) during Intense Storms (ISs) and Quiet time ered to be an important source of large Geomagnetically Substorms (QSs). SAPS occurred during 37 ISs and 30 Induced Currents (GICs) in middle- and low-latitude QSs were analyzed. Generally, SAPS occur after the power grids. In Zhang et al., [1], the extreme inter- southward turning of the Interplanetary Magnetic Field planetary shock of 23 July 2012 is simulated under the (IMF) with time lags of 0–1.5 h for ISs and 0–2.5 h for assumption that it had hit the Earth with the result indi- QSs. SAPS usually occurred 0–3 h after the beginning cating the shock-caused SC would be 123 nT. Based on of storm main phases and 0–2 h after the substorm ex- statistics, the occurrence frequency of SCs with ampli- pansion onsets. The lifetimes of SAPS are generally tudes larger than the simulated one is estimated to be longer than the durations of southward IMF and storm approximately 0.2% during the past 147 years on the main phases. During QSs, the lifetimes of SAPS are Earth. During this extreme event, the simulation indi- shorter than the duration of the ISs. Superposed epoch cates that dB/dt, which is usually used as a proxy for analysis shows different evolution patterns of SAPS GICs, at a dayside low-latitude substation would exceed during ISs and QSs. The results of this study provide 100nT/min; this is very large for low-latitude regions. both physical insight and constrains to modeling the They then assess the GIC threat level based on the magnetosphere-ionosphere-thermosphere coupling. simulated geomagnetic perturbations. The results indi- The geomagnetic activity, which refers to the distur- cate that the risk remains at low level for the low- bances of the Earth's magnetic field, is caused by solar latitude power network on a global perspective. How- eruption phenomena and is one of the important space ever, the GIC risk may reach moderate or even high weather processes. Variations of the geomagnetic field level for some equatorial power networks due to the have several time scales, of which the long-term varia- influence of the equatorial electrojet. Results of this tions of decades to centuries are caused by the Earth's study have substantial implications for risk management, crust and the short-term variations of seconds to years CAO Jinbin, et al. Magnetospheric Physics in China are resulted from solar activity. In recent years, increas- dawn. (3) During the rapid growth of the storm main ing statistical studies have demonstrated that there are phase, the Averaged Total Flux (ATF) of ENA-O con- significant correlations between geomagnetic and solar tinues to increase, while the ENA-H to decrease syn- activities and Earth's climatic change. The coupling chronously. Correspondingly, the ATF ratio of ENA-O between the geomagnetic field and the Earth's atmos- to ENA-H grows in a way of being roughly proportional pheric system has motivated the researchers to explore to the increase of the absolute value of the ring current National Report 2016 the effects of geomagnetic activity on the Earth's wea- index Dst. ther and climatic systems. The purpose of Jin et al., [3] Coronal Mass Ejection (CME)-driven or Corotating is to review the progress of the domestic and foreign Interaction Region (CIR)-driven storms can change the investigations on the influences of the geomagnetic ac- electron distributions in the radiation belt dramatically, tivity on climatic elements, to present the latest research which can in turn affect the spacecraft in this region or results, and to explore the characteristics and possible induce geomagnetic effects. The twin Van Allen Probes, mechanisms of the impact of the geomagnetic activity launched on 30 August 2012, orbit near the equatorial on climatic elements. This paper provides us with the plane and across a wide range of L* with apogee at 5.8 2018 basis for further investigations of the impact of geo- Re and perigee at 620 km. Electron data from Van Allen magnetic activity on the Earth's weather and climate, Probes MagEIS and REPT instruments have been * * finally achieving a comprehensive and objective under- binned every 6 h at L =3 (defined as 2.5<L <3.5), 4 standing on the relationship between the geomagnetic (3.5<L*<4.5), 5 (4.5<L*<5.5). The superposed epoch activity and climatic elements. analysis shows that (1) CME storms induce more elec- Applying the method of statistical fitting based on the tron flux enhancement at L*=3 for energy channels be- probability distribution features of Start Pulse Height low 1 MeV than CIR storms; (2) CME storms induce (STPH) excited by ENA’s secondary electron, a set of more electron flux enhancement at L*=4 and 5 in the programs has been developed to process the TWINS energy channels above 1 MeV than CIR storms; (3) CIR (Two Wide-angle Imaging Neutral-atom Spectrometers) storms induce more electron flux enhancement at L*=4 satellite Level-0 data aiming to separate compositions of and 5 in the energy channels below 1 MeV than CME oxygen and hydrogen in ENA. Therein a model of storms; (4) intense CME induce more than 50 times flux STPH distribution needed for making the separation is enhancement for the energy channel around 400 keV at set up by fitting the satellite calibration data to the theo- L*=3; (5) intense CIR induce more than 50 times flux retic formula in being. Implementing the separation enhancement for the energy channel around 200 keV at method to the TWINS satellite measured data during a L*=4. The results of Shen et al., [5] are consistent with a great magnetic storm, the respective ENA-H and ENA- general picture of enhanced convection over a longer O differential flux distributions with Line-Of-Sight period for CIR storms which increased flux closer to (LOS) have been obtained, as well as their evolution geosynchronous orbit consistent with earlier studies, with the storm main phase growth. Hu et al., [4] found while CME storms likely produce deeper penetration of that: (1) There are obvious differences in both magn- enhanced flux and local heating which is greater at itudes and distributions of differential fluxes between higher energies at lower L*. ENA-H and ENA-O, implying from a certain angle the Based on 7 years' observations from Time History of differences between fluxes of energetic O+ and H+ ions Events and Macroscale Interactions during Substorms as ENAs’ sources. (2) During the period approaching (THEMIS), Liu et al., [6] investigate the statistical dis- the storm main phase, ENA-H displays intense Low tribution of electric field Pc5 ULF wave power under Altitude Emissions (LAEs) which appear in the aurora different geomagnetic activities and calculate the radial and sub-aurora region before midnight, suggesting diffusion coefficient due to electric field, for outer ra- strong proton precipitation coming from plasma-sheet diation belt electrons. A simple empirical expression of and RC (Ring Current) region into the lower atmosphere is also derived. Subsequently, they compare to previous below exobase; while the oxygen has no obvious LAEs, D-LL models and find similar Kp dependence with the but showing intensive fluxes along LOSs that traverse model, which is also based on in situ electric field extensive RC region located mainly in the magnetic measurements. The absolute value of is constantly local time sectors of post-midnight, pre-dusk and around higher than, probably due to the limited orbital coverage ·155· SPACE SCIENCE ACTIVITIES IN CHINA of CRRES. The differences between and the commonly ergy conversion process in the magnetotail before it can used and models are significant, especially in Kp de- provide the earthward energy flux in the magnetotail for pendence and energy dependence. Possible reasons for this intense storm. The strongest energy transport ob- these differences and their implications are discussed. served by the nightside probes occurs in the main phase. The diffusion coefficient provided in this paper, which However, the strongest energy measured by the dayside also has energy dependence, will be an important con- satellites is in the recovery phase without intense activi- tributor to quantify the radial diffusion process of radia- ties, two hours later. Different features of the energy National Report 2016 tion belt electrons. transport in the three phases of the storm may be closely Using data from ground-based magnetometers and related to the different physical processes such as the HF Doppler sounder, Ouyang, et al., [7] study ULtralow energy entry, westward drift, particle injection or other Frequency (ULF) waves excited during the Storm Sud- potential mechanisms.
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