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Magnetic reconnection at the Earths magnetopause: CLUSTER spacecraft observations at different scale

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Title: Magnetic reconnection at the Earths magnetopause: CLUSTER spacecraft observations at different scale


1
Magnetic reconnection at the Earths
magnetopauseCLUSTER spacecraft observations at
different scales
  • Licentiate thesis
  • by
  • Alessandro Retinò
  • Department of Astronomy and Space Physics
  • Uppsala University

2
Motivation
  • Magnetic reconnection - an universal mechanism to
    transfer mass, momentum and energy across
    boundary layers in plasmas
  • Earths magnetosphere - the best laboratory to
    study
  • in-situ magnetic reconnection
  • Magnetic reconnection affects for long time large
    volumes in space (large scales) but it is fast
    initiated in small diffusion regions (small
    scales)
  • Cluster spacecraft first magnetospheric mission
    with multi-point measurements

3
Outline
  • The solar wind - Earth interaction
  • Magnetic reconnection basics
  • Reconnection at the Earths magnetopause
  • The Cluster mission
  • My contribute
  • Paper I - large scales
  • Paper II - small scales

4
The Earths magnetosphere
5
Magnetic reconnection in the magnetosphere
DR
DR
Day (2001)
IMF BZlt0
6
Magnetic reconnectionLaboratory, Sun,
Astrophysics
Solar flares
Hall effect during magnetic reconnection in a
laboratory plasma Ren (2005)
Accretion disks astrophysical jets
7
Magnetic reconnectionBasic ideas
  • It is a local process (initiated at small scales)
  • that
  • changes the magnetic connectivity of plasma
    elements
  • changes the global magnetic field topology
  • converts energy from magnetic fields to charged
    particles

8
Magnetic reconnectionDefinitions
2D steady-state (good approximation)
3D
DR
Priest Forbes (2000)
  • X-point where two separatrices meet
  • E along the X-line
  • Change in magnetic connectivity
  • (breaking frozen-in condition)
  • Plasma flow across separatrices
  • General Magnetic Reconnection
  • breakdown of magnetic connection
  • due to a localized non-idealness.
  • Necessary and sufficient condition

9
Magnetic reconnectionOur "definition"
  • Change in magnetic topology
  • Bn at the current sheet
  • E?0 in the diffusion region
  • Plasma transport across the current sheet
  • plasma distribution functions
  • plasma composition
  • Energy conversion from B to the plasma
  • plasma acceleration in the current sheet/boundary
    layer
  • plasma heating
  • Particle acceleration
  • strong localized E at boundaries
  • strong localized currents at boundaries

10
Magnetic reconnectionTheoretical models
inflow
outflow
Parker (1957), Sweet (1958)
Petscheck (1964)
  • Reconnection rate u0/uA0 Bn/B0
  • Alfvenic outflow ueuA0
  • Energy conversion WB ½ WK ½ WT
  • Reconnection rate too small!
  • Faster reconnection
  • Smaller diffusion region
  • Particle accelerate at shocks (separatrices)

11
Evidence at large scales Fluid
  • Walén test
  • (tangential balance stress)
  • Direct method
  • ?ut ?Bt /(µ0?)1/2
  • deHoffmann-Teller (HT) frame
  • u-uHT uA

Treumann Baumjohann (1996)
12
Evidence at large scales Kinetic
  • Magnetosheath boundary
  • layer (MSBL)
  • Transmitted magnetospheric
  • Incident magnetosheath
  • Reflected magnetosheath
  • Magnetospheric boundary
  • layer (BL)
  • Transmitted magnetosheath with uigtuHT
  • Incident magnetospheric
  • Reflected magnetospheric

Cowley (1995)
13
Evidence at small scales
  • Ion diffusion region
  • Electron diffusion region
  • Magnetic separatrices

Mozer (2002)
14
The CLUSTER mission
  • Europen Space Agency (ESA) cornerstone
  • 4 identical spacecraft at variable separation
  • For first time possible to distinguish between
    spatial and temporal structures
  • IRF-U main responsability EFW instrument
  • (Electric fields and waves)

15
Paper IMotivation
  • Continuity in time
  • Southward IMF YES
  • Northward IMF ?
  • Antiparallel vs component
  • remote,simulations component
  • in-situ ?

time
Reconnection is continuous if the reconnection
rate ?0
16
Paper IOverview
  • duskside MP
  • southern emisphere
  • tailward of the cusp
  • northward IMF

IMF
  • orbit SC configuration ideal
  • Large MP crossings over 4h
  • SC/3 local monitor in MSH

17
Paper IReconnection continuous for northward IMF
  • in-situ at MP
  • 4 hours continuous
  • northward IMF, By variable

18
Paper IComponent reconnection
  • measure magnetic
  • shear at X-line
  • jet reversals ? close to X-line
  • magnetic shear at X-line
  • 180º antiparallel
  • lt180º component

19
Summary Paper I Large scales
  • Magnetic reconnection continuous for hours under
    northward IMF
  • In-situ evidence of component reconnection

20
Paper IIMotivation
  • Microphysics of reconnection
  • Few detailed observations
  • Separatrices close to the X-line

21
Paper IIOverview
SC/3 only (small scales)
  • high resolution observations close to the X-line
  • separatrix region between magnetic separatrix and
    reconnection jet
  • distance from X-line lt 60?sh,i 3000 km (from
    comparison with simulations)

22
Paper IIThe separatrix region (SR)
  • magnetic separatrix identified as boundary in
    waves
  • SR 5 ?sh,i wide
  • inside SR few subregions ?sh,i wide
  • ESW at the boundary with jet but not inside the
    separatrix region
  • µ-FTE

3
2
1
bulge
ESW
jet
magnetic separatrix
23
Paper IIWave-particle interaction inside the SR
  • wave-particle interaction mainly from
    simulations
  • in observations need simultaneous high-time
    resolution wave and particle measurements
  • here best observations in the separatrix region
    (instrument limit resolution)
  • subregions different properties
  • good agreement with simulations

0 away from X-line 180 towards X-line
24
Paper IIA sketch of the separatrix region
  • SR and its subregions spatial structures
  • bulge (µ-FTE) temporal structure

25
Summary Paper II Small scales
  • A separatrix region several ion lenghts wide
    exists on the magnetospheric side of the
    magnetopause 60 ion lengths away from the
    X-line.
  • This region contains a few subregions each about
    one ion lenght wide.
  • These subregions are highly structured down to
    the Debye scale.
  • Comparison with numerical simulations indicates
    good agreement although some features observed at
    small scales are not resolved.

26
Future work
  • Reconnection continuous at large temporal scales.
    Also true at short temporal scales 1 s? Or
    intermittent instead? µ-FTEs maybe important.
  • Component or antiparallel reconnection at the
    magnetopause? More in-situ measurements of
    magnetic shear.
  • The microphysics of magnetic reconnection
  • X-line crossings
  • Evidence of ion and electron diffusion regions
  • Separatrix region crossings away from X-line
  • Energy conversion
  • Transport across
  • The relationship between the diffusion region and
    the separatrix region. Is the separatrix region a
    direct extension of the diffusion region far away
    from the X-line?
  • Comparison with reconnection magnetotail
    observations. Different boundary conditions and
    scales, same microphysics?
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