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Summer School Alpbach 2002 Plasma Entry into the Magnetosphere. Götz Paschmann MPE/ISSI. 3D View of the Magnetosphere. First Magnetopause Crossing, 1961. MP as Tangential (a) vs. Rotational (b) Discontinuity. Magnetopause with Cluster at 100 km Separation. Cluster at 100 km.
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Summer School Alpbach 2002Plasma Entry into the Magnetosphere Götz Paschmann MPE/ISSI
Magnetopause with Cluster at 100 km Separation Cluster at 100 km
Cluster Observes Reconnection Jets Cluster Reconnection Jets
Cluster Observes Nearly Continuous Reconnection Almost Continuous Reconnection
Flux Transfer Events Sporadic, localised reconnection between the magnetosheath and magnetospheric fields….. …..creates 2 tubes of magnetic flux peeling back across the dayside magnetopause…. …..allowing magnetosheath plasma to enter the magnetosphere along the flux tube…. …..and magnetospheric plasma to escape. CJ Owen et al., MSSL
C3 12 CuspEntry Cusp SuperDarn MHD Cluster C3 Ion Geotail + 10mn IMF 15:00 15:30 16:00 16:30 17:00 17:30 18:00 Time UT (HH:MM)
Lrec Cusp H = H0 sin q/2 H0 Erec q/2 H0 Cusp Flux – Polar Cap Potential Relation Contribution to polar cap potential: Particle flux into the magnetosphere: [Hill, 1979]
For nsh = 15 cm-3, Bsh = 20 nT, H0 = 10 RE : Example: For a = 0.1, Lrec = 40 RE: Previous estimates: 1026 s-1
Z Lsw Esw q/2 Hsw rec Esw q/2 View from Sun Hsw Bsw In the solar wind: Cross-Section
dmp Bbl Z R0 Vbl Y dbl View from the Sun Top View Diffusive Entry Schematic 2Hbl Terminator
Diffusive EntryFlux across the Magnetopause: For D = 109 m2/s, nsh = 15 cm-3, nbl = 10 cm-3 dmp = 500 km, R0 = 15 RE : Transport in LLBL: For Hbl = 15 RE, Vbl = 200 km/s: 9 kV
Burke et al., JGR, May, 1999: • sin2q/2 - dependence of Frec • base-potential F0 ? 25 keV Total polar-cap potential: FPC = Frec + F0 F0 = Fdiff - Fk Measured Potential BT 10.4 nT ¥ 6.1 nT +4.3 nT + 2.3 nT ~ 25 kV