tracing solar wind plasma entry into the magnetosphere using ti/te ratio
DESCRIPTION
Beno i t Lavraud CESR/CNRS/Université de Toulouse, France and the Cluster teams “remote” contribution to the ISSI meeting of Feb. 2009. Tracing solar wind plasma entry into the magnetosphere using Ti/Te ratio. At low SW Mach number the magnetosphere behaves very differently; effects include: - PowerPoint PPT PresentationTRANSCRIPT
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Benoit Lavraud CESR/CNRS/Université de Toulouse, France
and the Cluster teams
“remote” contribution to the ISSI meeting of Feb. 2009
Tracing solar wind plasma entry into the magnetosphere using Ti/Te ratio
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MOTIVATION: solar wind Mach number
At low SW Mach number the magnetosphere behaves very differently; effects include:
• Magnetosheath β properties
• Strong/asymmetric flows in magnetosheath
• Asymmetric magnetopause shape
• Cross Polar Cap Potential saturation
• Changes to dayside reconnection rate
• Alfvén wings/Sawtooth oscillations, …
And lower ion-to-electron temperature ratio in the magnetosheath
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MOTIVATION: Tracing plasma entry
Because magnetosheath ion-to-electron temperature ratio is lower during low Mach number (<6), I’ve been wondering whether one might use this property to trace SW plasma entry into the magnetosphere.
This presentation shows preliminary Cluster results that suggest we might indeed be able to do so…
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Magnetosheath flow acceleration and asymmetry
Asymmetric flow acceleration, along the flanks only: somewhat similar to a magnetic “slingshot”
Larger flows along flanks might enhance KH transport
Equatorial plane X = -5 RE
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Observation of such magnetosheath flow jets
Flows not associated with reconnection and 60% > SW
- Solar wind observations: IMF large and north SW density low
- Cluster observations: Flows B field outside MP Up to 1040 km/s while SW is only 650 km/s
Electrons
Ions
Sheath
sheathshock
dusk
Cluster
SW speed
Magnetopause
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Cluster overview of MP/sheath during the same day
Three clear boundary layer intervals with SW-like plasma inside the magnetopause
- Solar wind observations: Long low SW MA interval during a CME/MC
- Cluster observations: One clear instance of KH activity at MP/BL
Three clear boundary layer intervals in total
sheathshock
dusk
Cluster
Magnetopause
KH wave activityNo clear (N-Vx)roll-up
Boundary layerInside MP
Large sheath flows
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Temperature ratio observations for this interval
Ti/Te appears conserved for SW plasma in BL, instances where it is not conserved resemble pre-existing PS
Ti/Te NOT conserved
Ti/Te conserved
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CONCLUSIONS
• In this event, that BL contain SW plasma is obvious, although confirmed using this test as compared to inner PS plasma
• Possible future implications I would seek:- Determine which processes
(reconnection, KH, else?), if any, conserve this ratio during entry
- Trace entry into inner mag. regions (time-scales)
- How does this info get lost/destroyed? (drifts in inner regions, etc.)
Note: Cluster/THEMIS case around CME of Nov. 20, 2007
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EXTRA MATERIAL
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Magnetosheath flow dependence on Mach number
Strong flow acceleration : increasing for decreasing MA
Global MHD simulations (BATS-R-US)
for high and low Mach numbers
Illustration of strong sheath flows from Lavraud et al. [2007]
See also Chen et al. [1993], Rosenqvist et al. [2007]
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Movie of the field line « slingshot »
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Mechanism of magnetosheath flow acceleration
We can estimate the contribution of each force:J x B acceleration dominates at low Mach numbers
- Steady state momentum equation:
- Magnetic forces
- Integration of forces:
Selection of streamline
∂s
MHD simulation for low MA
Y (
RE)
Z (RE)
Bjpvv ).(
)2
().(1 2
B
BBBj
CurvBBp AAAs
v
Note: Not a simple analogy to a “slingshot”, magnetic pressure gradient as important as tension force(~10% 45% 45%)
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Observation of such magnetosheath flow jets
Flows not associated with reconnection and 60% > SW
- Solar wind observations: IMF large and north SW density low
- Cluster observations: Flows B field outside MP Up to 1040 km/s while SW is only 650 km/s
Electrons
Ions
Sheath
sheathshock
dusk
Cluster
SW speed
Magnetopause
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Flow asymmetry: role of IMF direction
The enhanced flow location follows the IMF orientation+ additional anomalous flow deflections [Nishino et al., 2008]
Flow magnitude and sample field lines from MHD simulations (X = -5 RE)
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Acknowledgments
Aaron J. Ridley (Univ. Michigan, USA)Janet Kozyra (Univ. Michigan, USA)Maria M. Kuznetsova and CCMC
(NASA GSFC, USA)and Cluster teams