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Problems in Space Physics 長井嗣信 東京工業大学. 磁気圏の未解決問題 「いつも同じ話をしている」 1.容易に解決できそうだが 2.何が観測的に問題なのか 3.今後どうすべきか.

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Presentation on theme: "Problems in Space Physics 長井嗣信 東京工業大学. 磁気圏の未解決問題 「いつも同じ話をしている」 1.容易に解決できそうだが 2.何が観測的に問題なのか 3.今後どうすべきか."— Presentation transcript:

1 Problems in Space Physics 長井嗣信 東京工業大学

2 磁気圏の未解決問題 「いつも同じ話をしている」 1.容易に解決できそうだが 2.何が観測的に問題なのか 3.今後どうすべきか

3 1.Substorm Onsets 2.Magnetic Storms 3.Plasma Convection

4 1.Substorm Onsets Global Images Intense Ground Observation Network Mid-Tail Observations 10-30 Re Geosynchronous Orbit 6.6 Re

5 L. A. Frank ICS-4 (1998) January 12, 1997 0726 UT

6 Polar/UVI by A. Ieda0725:11 UT

7 Polar/UVI January 12, 1997 0724:54 UT

8 0725 UT

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10 0723 UT

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14 Gang Lu JGR 1999

15 Gang Lu JGR 1999 70

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17 Kadokura (2002) SIT-TV at Syowa 427.8 nm

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19 Problems 1.Spatial Resolution 2.Time Resolution 3.UV 4.Magnetic Field Tracing 5.Conjugate Events

20 L. R. Lyons et al. JGR 2001

21 L. R. Lyons et al., JGR 2001

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23 10E 71.3 E 105E 141 E 192.5 E 322.5E Geographic Longitude Geomag. Lat. 1.5 -8.3 -10.4 -8.7 -1.1 8.6

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28 Global Satellite Aurora Images Spatial Resolution Time Resolution UV Comparison with Ground Observations Geosynchronous Substorm Signatures Longitudinal Effect Particles or Magnetic Field

29 McPherron 1991Kamide and Baumjohann 1993

30 Burton et al., 1975 2.Magnetic Storms

31 Ring Current Modeling Ebihara et al. 2001, 2002

32 Strangeway and Johnson 1983

33 Strangeway and Johnson 1983

34 Strangeway and Johnson 1983

35 Magnetic Storms 1.Solar wind parameters Dst 2.Ring current modeling (dipole field) Dst 3.H+ vs. O+ 4.What should be known? Particle distributions Time, Position (L, MLT, Latitude) Energy, Species

36 3. Plasma Convection Plasma Transport = Field Transport Pictures from Ground Observations Pictures from Tail Observations

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38 Polar Cap Potential Drop 100 kV Polar Cap > 75 degrees L = 2 x 3.14 x 6371.2 x 30/360 = 3300 km E = 100kV / 3300km = 30 mV/m B = 60000 nT V = E/B = 30 mV/m / 60000 nT = 500 m/s T = 3300km / 500 m/s = 100 min Vsw = 500 km/s T = 100 Re/500 km/s = 20 min

39 Nishitani et al. JGR 2001

40 Plasma Convection in the Tail Stationary vs Bursty Paterson et al. JGR 1998 100 Re/10 km/s = 1000 min Angelopoulos et al. 1999

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45 A dipolarization at 10 Re (for a substorm)

46 Mid- and Near-Tail Plasma Observations 1.Plasmas are NOT MHD 2.Problems in the Present Instruments No Convincing Observations

47 今後の方向 1.確かに進歩 2.新たな問題 3.根本的な問題 将来計画 1.対象の明確化(絞込み) 2.何が必要とされているか 3.対象にあった観測 機械と軌道

48 4.IMF Bz Control for the Plasma Sheet 1.IMF Bz > 0 (northward) 2.IMF Bz < 0 (southward) 3.ssc (density increase in SW)

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54 IMF Bz Effect Substorms IMF Bz Northward Turning > 50% IMF Bz > 0 Substorm Processes Prolonged IMF Bz Periods Cold and Dense Plasmas Stationary

55 Summary 1.Importance of Ground Observations Optical Aurora 2.Ionospheric Signatures North / South Conjugate 3.IMF Bz Control Drastic Changes

56 Future Mission SCOPE (Scale Coupling in Plasma Environment) 1.High time resolution in particle observations 2.Full energy coverage in particle observations 3.Multi-point observations to know the s/c location relative to the neutral line


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