Observations of a structured ionospheric outflow plume at Titan EGU General Assembly Vienna, Austria 3-8 April 2011 Z66 EGU2011 1356 Abstract Recent results.

Slides:



Advertisements
Similar presentations
G. Marklund Space & Plasma Physics, School of Electrical Engineering, KTH Stockholm, Cluster multi-probing of the aurora above and within the acceleration.
Advertisements

Dusty plasma near Enceladus South Pole M. Shafiq, M. W. Morooka and J.-E. Wahlund Swedish Institute of Space Physics, Uppsala, Sweden.
Reconnection at Ganymede: Work in Progress Bill Paterson & Glyn Collinson NASA GSFC.
Towards Low-cost Swedish Planetary Missions S. Barabash 1, O. Norberg 2, J.-E. Wahlund 3, M. Yamauchi 1, S. Grahn 4, S. Persson 4, and L. Blomberg 5 1.
Lundstedt (IRF-Lund). Narayan (Stockholm-U) Kanao (ISAS, Japan) The effect of the crustal magnetic field on the distribution of the ion number density.
Surface Penetrating Radar Simulations for Jupiter’s Icy Moons Thorsten Markus, Laboratory for Hydrospheric Processes NASA/GSFC,
Near-Earth Magnetotail Reconnection and Plasmoid Formation in Connection With a Substorm Onset on 27 August 2001 S. Eriksson 1, M. Oieroset 2, D. N. Baker.
Anti-parallel versus Component Reconnection at the Magnetopause K.J. Trattner Lockheed Martin Advanced Technology Center Palo Alto, CA, USA and the Polar/TIMAS,
Which describes a variation of wave frequency ω(t) in a geometric-optic approximation [4]. Here n(ω) is the refractive index of the medium, is the vector.
Five Spacecraft Observations of Oppositely Directed Exhaust Jets from a Magnetic Reconnection X-line Extending > 4.3 x 10 6 km in the Solar Wind Gosling.
Summer student work at MSSL, 2009 Kate Husband – investigation of magnetosheath electron distribution functions. Flat-topped PSD distributions, correlation.
HF Focusing due to Field Aligned Density Perturbations A. Vartanyan 1, G. M. Milikh 1, K. Papadopoulos 1, M. Parrot 2 1 Departments of Physics and Astronomy,
Ionospheric photoelectrons at Venus: ASPERA-4 observations A.J. Coates 1,2 S.M.E. Tsang 1,2, R.A. Frahm 3, J.D. Winningham 3, S. Barabash 4, R. Lundin.
In-situ Observations of Collisionless Reconnection in the Magnetosphere Tai Phan (UC Berkeley) 1.Basic signatures of reconnection 2.Topics: a.Bursty (explosive)
Magnetic Reconnection Rate and Energy Release Rate Jeongwoo Lee 2008 April 1 NJIT/CSTR Seminar Day.
Electrons at Saturn’s moons: selected CAPS-ELS results A.J. Coates 1,2. G.H. Jones 1,2, C.S.Arridge 1,2, A. Wellbrock 1,2, G.R. Lewis 1,2, D.T. Young 3,
Numerical simulations are used to explore the interaction between solar coronal mass ejections (CMEs) and the structured, ambient global solar wind flow.
CLUSTER Electric Field Measurements in the Magnetotail O. Marghitu (1, 3), M. Hamrin (2), B.Klecker (3), M. André (4), L. Kistler (5), H. Vaith (3), H.
Concentrated Generator Regions in the Auroral Magnetosphere as Derived from Conjugated Cluster and FAST Data M. Hamrin (1),O. Marghitu (2, 3), B.Klecker.
NOSCI Infrastructure for Lunar Observatories Bremen, Germany March 22 – 24, 2005 NanOspace-1 SCientific Instruments Jan Bergman Swedish Institute of Space.
Remote Radio Sounding Science For JIMO J. L. Green, B. W. Reinisch, P. Song, S. F. Fung, R. F. Benson, W. W. L. Taylor, J. F. Cooper, L. Garcia, D. Gallagher,
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Classical electrodynamics.
1 Proximal +/- 1 hr Priorities June 5, 2014 RPWS Team Science Priorities (+/- 1 hr) W. Kurth and D. A. Gurnett For the RPWS Team Cassini PSG Telecon 5.
Negative ions at Titan: tholins for Titan’s haze? Andrew Coates, Mullard Space Science Laboratory, UCL, UK With thanks to Frank Crary, Dave Young, Hunter.
Structure and dynamics of induced plasma tails César L. Bertucci Presented by Oleg Vaisberg Institute for Astronomy and Space Physics, Buenos Aires, Argentina.
Multi-fluid MHD Study on Ion Loss from Titan’s Atmosphere Y. J. Ma, C. T. Russell, A. F. Nagy, G. Toth, M. K. Dougherty, A. Wellbrock, A. J. Coates, P.
Large-Amplitude Electric Fields Associated with Bursty Bulk Flow Braking in the Earth’s Plasma Sheet R. E. Ergun et al., JGR (2014) Speaker: Zhao Duo.
Coronal Sources of Impulsive Fe-Rich Solar Energetic Particle Events S. W. Kahler AFRL Space Vehicles Directorate, Kirtland AFB, NM, USA D. V. Reames IPST,
MOP 2011, BOSTON, MA, USAJuly 14, 2011 Norbert Krupp Open-Close Field line Boundary Characterization of Saturn‘s magnetosphere using Cassini MIMI-LEMMS.
Space Science MO&DA Programs - September Page 1 SS It is known that the aurora is created by intense electron beams which impact the upper atmosphere.
References: [1]S.M. Smith et al. (2004) Advances in functional and structural MR image analysis and implementation in FSL. Neuroimage 23: [2]S.M.
The state of the plasma sheet and atmosphere at Europa D. E. Shemansky 1, Y. L. Yung 2, X. Liu 1, J. Yoshii 1, C. J. Hansen 3, A. Hendrix 4, L. W. Esposito.
Cold plasma: a previously hidden solar system particle population Mats André and Chris Cully Swedish Institute of Space Physics, Uppsala.
Influence of negatively charged plume grains on the structure of Enceladus' Alfven wings: hybrid simulations versus Cassini MAG data Hendrik Kriegel
1 The Organic Aerosols of Titan’s Atmosphere Christophe Sotin, Patricia M. Beauchamp and Wayne Zimmerman Jet Propulsion Laboratory, California Institute.
Saturn neutral particle modeling Overview of Enceladus/Titan research with possible application to Mercury Johns Hopkins University Applied Physics Laboratory.
INMS quarterly report: Aug.-Sept., 2005 Science highlights –In situ determination of the atmosphere of Enceladus much beyond anticipation - water 90%,
Plasmasphere Refilling Rates Inferred from Polar and IMAGE Satellite Spectrogram Data T. Huegerich(1), J. Goldstein(1), P.H. Reiff(1), B.W. Reinisch(2)
5. Walen Test analysis The Walen Test results for Cluster 3 are as expected for a reconnection event. The test over the leading edge shows a positive correlation.
Cluster observations of a reconnection site at high- latitude magnetopause Y. Khotyaintsev (1), A. Vaivads (1), Y. Ogawa (1,2), M. André(1), S. Buchert(1),
Nicola Patmore & Ralf Toumi (contact: Space and Atmospheric Physics Group, Imperial College London Abstract A Tropopause.
Simple Approach to Salvaging THEMIS ESA Moments Prior to Boom Deployment Vladimir Kondratovich David G. Sibeck.
A. Vaivads, M. André, S. Buchert, N. Cornilleau-Wehrlin, A. Eriksson, A. Fazakerley, Y. Khotyaintsev, B. Lavraud, C. Mouikis, T. Phan, B. N. Rogers, J.-E.
1 Hybrid Simulations of the Callisto - Magnetosphere Interaction Stas Barabash and Mats Holmström Swedish Institute of Space Physics, Kiruna, Sweden.
Relating the Equatorward Boundary of the Diffuse Redline Aurora to its Magnetospheric Counterpart Grant, Jeff 1 ; Donovan, Eric 1 ; Spanswick, Emma 1 ;
A. J. Kopf 1,2 and D. A. Gurnett 1 1 University of Iowa 2 University of Florida Special thanks to J. D. Menietti, R. L. Mutel, and W. M. Farrell.
Catalogued parameters… Current sheet normal vector and velocity, derived using a timing analysis. Later used to calculate an accurate measure of current.
Saturn’s field aligned currents and their modulation by the Planetary Period Oscillations Greg Hunt 1 *, S. W. H. Cowley 1, G. Provan 1, E. J. Bunce 1,
RPWI Team Meeting, Sep. 2010, Roma Magnetic Loop Antenna (MLA) Scientific Objectives A. Marchaudon, V. Krasnoselskikh, T. Dudok de Wit, C. Cavoit,
Krusenberg Herrgård 12 June 2007 L Nordh/Mats André Swedish Report to ILWS.
M. Yamauchi 1, H. Lammer 2, J.-E. Wahlund 3 1. Swedish Institute of Space Physics (IRF), Kiruna, Sweden 2. Space Research Institute (IWF), Graz, Austria.
Radio and Space Plasma Physics Group Tracking solar wind structures from the Sun through to the orbit of Mars A.O. Williams 1, N.J.T. Edberg 1,2, S.E.
The large scale convection electric field, ring current energization, and plasmasphere erosion in the June 1, 2013 storm Scott Thaller Van Allen Probes.
Impact of CIRs/CMEs on the ionospheres of Venus and Mars Niklas Edberg IRF Uppsala, Sweden H. Nilsson, Y. Futaana, G. Stenberg, D. Andrews, K. Ågren, S.
二维电磁模型 基本方程与无量纲化 基本方程. 无量纲化 方程化为 二维时的方程 时间上利用蛙跳格式 网格划分.
Effects of January 2010 stratospheric sudden warming in the low-latitude ionosphere L. Goncharenko, A. Coster, W. Rideout, MIT Haystack Observatory, USA.
SS Special Section of JGR Space Physics Marks Polar’s 5th Anniversary September 4, 1996 This April special section is first of two Polar special sections.
R. Maggiolo 1, M. Echim 1,2, D. Fontaine 3, A. Teste 4, C. Jacquey 5 1 Belgian Institute for Space Aeronomy (IASB-BIRA); 2 Institute.
AGILE as particle monitor: an update
Figure 3. The hybrid simulations results
M. Yamauchi1, I. Dandouras2, H. Reme2,
Inside Jupiter and Saturn
Field aligned density perturbations and ion outflows at HAARP
Background for JGO: Rosetta dual Langmuir probes (LAP)
Exploring the ionosphere of Mars
Blowing magnetic skyrmion bubbles
Model Calculations of the Ionosphere of Titan during Eclipse Conditions Karin Ågren IRF-U, LTU.
Fig. 1 Solar cycle and experimental setup.
Radar Soundings of the Ionosphere of Mars
by Andreas Keiling, Scott Thaller, John Wygant, and John Dombeck
Presentation transcript:

Observations of a structured ionospheric outflow plume at Titan EGU General Assembly Vienna, Austria 3-8 April 2011 Z66 EGU Abstract Recent results obtained from measurements by the Cassini Radio and Plasma Wave Science/Langmuir probe (RPWS/LP), magnetometer (MAG) and electron sensor (ELS) instruments are presented. We study the structured outflow of ionospheric plasma from the induced magnetosphere of Titan. During the final three of the five consecutive and similar Cassini Titan flybys T55 - T59 we observe a region characterized by high electron densities (1-8 cm -3 ) in the tail/night side of Titan. Both light and heavy ions with ionospheric composition are observed to travel away from Titan in this region. This region is observed progressively farther downtail from pass to pass and is interpreted as a plume of ionospheric plasma escaping Titan, which appears steady in both location and time. It extends to at least 6 Titan radii downstream of the moon. Magnetic field measurements indicate the presence of a current sheet at the inner edge of this region. We discuss the mechanism behind this outflow, and suggest that ambipolar diffusion, magnetic moment pumping or dispersive Alfvén waves could cause it. Niklas Edberg, K. Ågren, J.-E. Wahlund, M. W. Morooka IRF, Uppsala, Sweden D. J. Andrews, S. W. H. Cowley University of Leicester, UK A.Wellbrock, A. J. Coates MSSL University College London, UK C. Bertucci IAFE, Buenos-Aires, Argentina M. K. Dougherty Imperial College London, UK Acknowledgements NJTE was supported the Swedish Research Council. Contact: References N.J.T. Edberg et al., Planet. Space. Sci, 2011 (in press) Fig 6. Cassini flyby configuration for the T flybys (thin red lines). The thick red lines on top of the T55 and T56 tracks indicate the region of an extended ionosphere. The thick red lines on top of the T57, T58 and T59 tracks indicate the interval when the density plume is observed (see Figure 1-5). The blue lines show the average components of the magnetic field for each flyby. Fig 1-5. Cassini RPWS, MAG, and ELS data from the T55-T59 flybys shown as a time series. The panels show from top to bottom: the LP voltage-current characteristics, LP measured N e (blue) together with N e derived from F UH emisions (red), LP measured T e, LP floating potential (cyan) and LP spacecraft potential (blue), MAG vector magnetic fields in TIIS coordinates, and an ELS electron spectrogram. T55 T56 T57 T58 T59 T55 T56 T57 T58 T59 Summary Ionospheric plasma is observed to escape in a structured plume during the Cassini T55-T59 flyby. N e = 1-8 cm -3 in the plume. The plume consists of light and heavy ions with composition indicating that it comes from Titan’s ionosphere. Ions move in direction away from Titan and hence are escaping. e - have isotropic distribution. The plume extends to > 6 R T behind the moon. Fig 7. Altitude profiles of the electron density measured during the inbound legs of the T55-T59 flybys. The observations of the electron plume are highlighted by the shaded regions.