14 May 20131 JIM M. RAINES University of Michigan DANIEL J. GERSHMAN, THOMAS H. ZURBUCHEN, JAMES A. SLAVIN, HAJE KORTH, and BRIAN J. ANDERSON Magnetospheric.

Slides:



Advertisements
Similar presentations
MURI,2008 Electric Field Variability and Impact on the Thermosphere Yue Deng 1,2, Astrid Maute 1, Arthur D. Richmond 1 and Ray G. Roble 1 1.HAO National.
Advertisements

Hydrogen Hot Ion Precipitation in the Martian Ionosphere #P13B-1317 Christopher D. Parkinson 1, Michael Liemohn 1, Xiaohua Fang 2 1 AOSS Dept., University.
Evidence at Saturn for an Inner Magnetospheric Convection Pattern, Fixed in Local Time M. F. Thomsen (1), R. L. Tokar (1), E. Roussos (2), M. Andriopoulou.
Plasma layers in the terrestrial, martian and venusian ionospheres: Their origins and physical characteristics Martin Patzold (University of Cologne) and.
Magnetopause flow vortices revealed during high speed solar wind streams Mona Kessel (NASA GSFC), Yaireska Collado-Vega (University of Puerto Rico), Xi.
Comparing the solar wind-magnetosphere interaction at Mercury and Saturn A. Masters Institute of Space and Astronautical Science, Japan Aerospace Exploration.
Space Weather. Coronal loops Intense magnetic field lines trap plasma main_TRACE_loop_arcade_lg.jpg.
Auxiliary slides. ISEE-1 ISEE-2 ISEE-1 B Locus of  = 90 degree pitch angles Will plot as a sinusoid on a latitude/longitude projection of the unit.
Plasma entry in the Mercury’s magnetosphere S. Massetti S. Massetti INAF-IFSI Interplanetary Space Physics Institute, Roma - Italy.
Auroral dynamics EISCAT Svalbard Radar: field-aligned beam  complicated spatial structure (
Morphology of meteoric plasma layers in the ionosphere of Mars as observed by the Mars Global Surveyor Radio Science Experiment Withers, Mendillo, Hinson.
Solar wind interaction with the comet Halley and Venus
Summer student work at MSSL, 2009 Kate Husband – investigation of magnetosheath electron distribution functions. Flat-topped PSD distributions, correlation.
Or A Comparison of the Magnetospheres between Jupiter and Earth.
Reinisch_ Solar Terrestrial Relations (Cravens, Physics of Solar Systems Plasmas, Cambridge U.P.) Lecture 1- Space Environment –Matter in.
In-situ Observations of Collisionless Reconnection in the Magnetosphere Tai Phan (UC Berkeley) 1.Basic signatures of reconnection 2.Topics: a.Bursty (explosive)
Magnetospheric Morphology Prepared by Prajwal Kulkarni and Naoshin Haque Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global.
Mercury’s Atmosphere: A Surface-bound Exosphere Virginia Pasek PTYS 395.
November 2006 MERCURY OBSERVATIONS - JUNE 2006 DATA REVIEW MEETING Review of Physical Processes and Modeling Approaches "A summary of uncertain/debated.
Tuija I. Pulkkinen Finnish Meteorological Institute Helsinki, Finland
Benoit Lavraud CESR/CNRS, Toulouse, France Uppsala, May 2008 The altered solar wind – magnetosphere interaction at low Mach numbers: Magnetosheath and.
A TMOSPHERIC, O CEANIC AND S PACE S CIENCES UNIVERSITY of MICHIGAN Daniel J. Gershman, James A. Slavin, Jim M. Raines, Thomas H. Zurbuchen, Brian J. Anderson,
Copyright © 2010 Pearson Education, Inc. The Jovian Planets Jupiter, Saturn, Uranus, Neptune.
Atmospheres of the Planets By Danielle Stroup. Introduction-Definitions Atmosphere consists of molecules and atoms moving at various speeds Temperature.
Chapter 17.1 Atmospheric Characteristics
Negative Ions in IEC Devices David R. Boris 2009 US-Japan IEC Workshop 12 th October, 2009 This work performed at The University of Wisconsin Fusion Technology.
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.
The PLANETOCOSMICS Geant4 application L. Desorgher Physikalisches Institut, University of Bern.
Foreshock studies by MEX and VEX FAB: field-aligned beam FAB + FS: foreshock M. Yamauchi et al.
9 May MESSENGER First Flyby Magnetospheric Results J. A. Slavin and the MESSENGER Team BepiColombo SERENA Team Meeting Santa Fe, New Mexico 11 May.
Solar Wind and Coronal Mass Ejections
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Spring, 2012 Copyright © The Heliosphere: The Solar Wind March 01, 2012.
1 Mars Micro-satellite Mission Japanese micro-satellite mission to Mars to study the plasma environment and the solar wind interaction with a weakly-magnetized.
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.
Initial Measurements of O-ion and He-ion Decay Rates Observed from the Van Allen Probes RBSPICE Instrument Andrew Gerrard, Louis Lanzerotti et al. Center.
In Situ Measurements of Auroral Acceleration Regions Wu Tong
Low-energy Suprathermal Electrons in Mercury’s Magnetosphere George C. Ho, Richard D. Starr, Jon D. Vandegriff, Stamatios M. Krimigis, Robert E. Gold,
Cold plasma: a previously hidden solar system particle population Mats André and Chris Cully Swedish Institute of Space Physics, Uppsala.
Ionospheric Current and Aurora CSI 662 / ASTR 769 Lect. 12 Spring 2007 April 24, 2007 References: Prolss: Chap , P (main) Tascione: Chap.
ESS 7 Lecture 13 October 29, 2008 Substorms. Time Series of Images of the Auroral Substorm This set of images in the ultra-violet from the Polar satellite.
2001/02/08T E Moore - SW Interactions via LENA1 Solar Wind-Magnetosphere Interactions via Low Energy Neutral Atom Imaging T E Moore[1], M R Collier[1],
1 MAVEN PFP ICDR May 23-25, 2011 Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission Particles and Fields Science Critical Design Review May ,
PARTICLES IN THE MAGNETOSPHERE
Mass Transport: To the Plasma Sheet – and Beyond!
Analysis of Suprathermal Events Observed by STEREO/PLASTIC with a Focus on Upstream Events STEREO SWG - 20 Meredith, NH October 27-29, 2009 Josh Barry,
NASA NAG Structure and Dynamics of the Near Earth Large-Scale Electric Field During Major Geomagnetic Storms P-I John R. Wygant Assoc. Professor.
17th Cluster workshop Uppsala, Sweden , May 12-15, 2009
Image credit: NASA Response of the Earth’s environment to solar radiative forcing Ingrid Cnossen British Antarctic Survey.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 7 The Jovian Planets.
The Suprathermal Tail Properties are not well understood; known contributors Heated solar wind Interstellar and inner source pickup ions Prior solar and.
Magnetospheric Current System During Disturbed Times.
The effects of the solar wind on Saturn’s space environment
MULTI-INSTRUMENT STUDY OF THE ENERGY STEP STRUCTURES OF O + AND H + IONS IN THE CUSP AND POLAR CAP REGIONS Yulia V. Bogdanova, Berndt Klecker and CIS TEAM.
© Research Section for Plasma and Space Physics UNIVERSITY OF OSLO Daytime Aurora Jøran Moen.
SEPT/STEREO Observations of Upstream Particle Events: Almost Monoenergetic Ion Beams A. Klassen, R. Gomez-Herrero, R. Mueller-Mellin and SEPT Team, G.
ASEN 5335 Aerospace Environments -- Magnetospheres 1 As the magnetized solar wind flows past the Earth, the plasma interacts with Earth’s magnetic field.
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.
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.
Observations of reflected ions downstream of shocks in the heliosphere John Richardson M.I.T. (Voyager plasma experiment) 10 – 5950 eV/q.
A Global Hybrid Simulation Study of the Solar Wind Interaction with the Moon David Schriver ESS 265 – June 2, 2005.
Source and seed populations for relativistic electrons: Their roles in radiation belt changes A. N. Jaynes1, D. N. Baker1, H. J. Singer2, J. V. Rodriguez3,4.
1. What controls the occurrence of reconnection. 2
© 2017 Pearson Education, Inc.
High-latitude Neutral Density Maxima
MESSENGER observations of Mercury’s northern cusp
THEMIS multi-spacecraft observations of a 3D magnetic
PLANETARY X-RAY AURORAS
Chapter 7 The Jovian Planets
Energy conversion boundaries
Magnetosphere: Structure and Properties
Presentation transcript:

14 May JIM M. RAINES University of Michigan DANIEL J. GERSHMAN, THOMAS H. ZURBUCHEN, JAMES A. SLAVIN, HAJE KORTH, and BRIAN J. ANDERSON Magnetospheric Cusp Structure and Dynamics: MESSENGER FIPS Measurements at Mercury

Previous results 14 May FIPS measurements show highest concentration of planetary ions in cusp [Zurbuchen et al. 2011] Size of Mercury’s cusp [Winslow et al. 2012] more like Earth’s outer cusp Na + -group ions are ~2 times more abundant than solar wind He 2+ in the cusp area on the average [Raines et al., 2012] Jim M. Raines, Univ. of Michigan Updated version from Zurbuchen et al., 2011

Produced in the cusp by solar wind sputtering from the surface Solar wind Na + Produced upstream (magnetosheath and beyond) and driven into the cusp Na Na + hν Driving Question 14 May 20133Jim M. Raines, Univ. of Michigan Where and how are the Na + -group ions observed in and around the cusp produced?

REPRESENTATIVE CUSPS 14 May 20134Jim M. Raines, Univ. of Michigan

Typical case 1: Expected cusp 14 May 20135Jim M. Raines, Univ. of Michigan Small spatial extent Na + -group ions grouped with protons Na + -group ions >1 keV (energies vary) cusp QUIET cusp

Typical case 3: Active 6 Hot Na + -group ions, mostly > 2keV Low energy bins below detection threshold at these low densities Dayside Na + -group ions FTEs ACTIVE cusp 14 May 2013Jim M. Raines, Univ. of Michigan

Active with lots of Na+, low E dayside 14 May 20137Jim M. Raines, Univ. of Michigan Colder ions at lower LAT than cusp Hot ions in cusp FTEs Trapped in dayside closed-field region? ~55 km gyroradius at equator is small enough to fit inside dayside magnetosphere Atypical: Low energy Na +

COLLECTIVE PROPERTIES 14 May 20138Jim M. Raines, Univ. of Michigan

Cusp Na + -group Properties Surveyed 518 cusp crossings, Sept 2011 – May Significant in ~30% of cusps –Active (~20%), has significant dayside component –Quiet (~10%), NO significant dayside component Peak ~900 km altitude ~ 2.7 keV Low energy, eV, <1% of observed particles (in <5% of cusp crossings) Most active and highest energies coincident with FTE activity 14 May 20139Jim M. Raines, Univ. of Michigan LAT only

Na + -group Pitch Angle Distributions 14 May Jim M. Raines, Univ. of Michigan Not consistent with beaming distributions QuietActiveActive (dayside portion)

Seasonal Variability 14 May Jim M. Raines, Univ. of Michigan Cusp only: LAT LT 9-15

Seasonal Variability (2) 14 May Jim M. Raines, Univ. of Michigan Cusp only: LAT LT 9-15 TAA ~135 TAA ~240 Z MSO (R M ) Y MSO (R M ) X MSO (R M ) Na + -group ion variability shows patterns with TAA TAA and LT of periapsis are phased locked Variability could be seasonal (TAA) or spatial (LT)

DISCUSSION 14 May Jim M. Raines, Univ. of Michigan

Acceleration Mechanisms Initial ion energy <10 eV from direct surface processes or photoionization Local to cusp –Centrifugal from E x B drift »Cleft ion fountain observed at Earth »Predicted at Mercury »Can accelerate to 10x initial energy but only a small fraction within cusp –Wave-particle interactions »Can accelerate up to 10-20x initial energy –Not enough for 10 eV  2.7 keV Away from cusp –Solar wind pickup »160 km/s magnetosheath flow gives 3-12 keV Na + –Dayside reconnection »3 keV in range for Alfven speed expected from outflow 14 May Jim M. Raines, Univ. of Michigan Delcourt et al., 2012 Na + trajectories in the X-Z plane. The test ions are launched from the planet surface at 65 latitude in the dayside sector, with 0.01 eV or 0.1 eV energy, 170 pitch angle and arbitrary gyrophase. Blue, green and orange-red colors correspond to cross-polar cap potential drops of 2 kV, 5 kV, and 10 kV, respectively. Adapted from Delcourt et al., 2012.

Circulation? Could < 10 eV Na + ions be accelerated into the tail then circulate back to the cusp with keV energies? 14 May Jim M. Raines, Univ. of Michigan Small clearance within dayside magnetosphere makes circulation by >2 keV ions unlikely. Ions in the 200 eV range do fit – energy filter?

Source of Na + -group Ions Na is ionized in the magnetosheath (and beyond) and the resulting Na + -group ions are swept into the cusp Majority of Na + -group ions observed >2 keV Observed energies consistent with ion pickup or reconnection heating Dayside component and association with magnetic activity may mean FTEs are carrying ions into cusp Na + -group ions are sputtered off of the surface at low energy, < 10 eV, by solar wind ions funneling down the cusp. Known local heating/acceleration mechanisms cannot account for high energy (> 2 keV) of observed ions Observed density maximum is in upper half of cusp altitudes Pitch angles do not show beaming up from surface Low energy ( eV) Na + - group ions observed only in minority of cusps (< 5%) 16 Strongly indicated 14 May 2013Jim M. Raines, Univ. of Michigan

Summary and Conclusions Na + -group ions are routinely observed in the cusp region with energies of keV and observed densities of cm -3. Na + -group ions in the cusp show substantial variability. The highest densities and energies of Na + -group ions correlate with magnitude of diamagnetic decrease and level of FTE activity. The high energies (2-4 keV) of Na + group ions regularly observed in the cusp strongly favor ionization in the magnetosheath (and beyond) then sweeping into the cusp, possibly by reconnection. Low energy ( eV) Na + ions are occasionally present at lower dayside latitudes than the cusp. These ions may be accelerated locally, recirculated from the magnetotail and/or trapped in the closed-field dayside magnetosphere. 14 May Jim M. Raines, Univ. of Michigan

Jupiter and Mercury, 13 Mar Image: Pete Lawrence via NASA. 14 May 2013Jim M. Raines, Univ. of Michigan18