October 8 2013 CME Shock Event Hudson, Paral, Kress, Turner SWE ACE Solar Wind Electron Proton Alpha Monitor K0>5-Min ---------------------------------------------

Slides:



Advertisements
Similar presentations
S. Elkington, GEM 2003 Transport in the Radiation Belts and the role of Magnetospheric ULF Waves Scot R. Elkington LASP, University of Colorado With many.
Advertisements

First composition measurements of energetic neutral atoms A. T. Y. Lui et al., GRL, Vol 23, pages: , 1996.
Waves and Particles in the Radiation Belt Kaiti Wang PSSC/NCKU March 17, 2009 Opportunity for Collaboration on ERG and SCOPE Missions & Community Input.
Electron Acceleration in the Van Allen Radiation Belts by Fast Magnetosonic Waves Richard B. Horne 1 R. M. Thorne 2, S. A. Glauert 1, N. P. Meredith 1.
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.
First panel is the EFW spin fit (10.5 s) electric field in ~ dawn-dusk direction. This measurement is dominated by waves with amplitudes >32 mV/m ptp during.
The Importance of Wave Acceleration and Loss for Dynamic Radiation Belt Models Richard B. Horne M. M. Lam, N. P. Meredith and S. A. Glauert, British Antarctic.
ESS 7 Lecture 14 October 31, 2008 Magnetic Storms
Jasper S. Halekas Space Sciences Laboratory
Radiation Belt Loss at the Magnetopause T. G. Onsager, J. C. Green, H. J. Singer, G. D. Reeves, S. Bourdarie Suggest a pitch-angle dependence of magnetopause.
Cusp Radiation Source: A Challenge for Theory and Simulation Jiasheng Chen, Theodore A. Fritz, Katherine E. Whitaker, Forrest S. Mozer, and Robert B. Sheldon.
Anti-parallel versus Component Reconnection at the Magnetopause K.J. Trattner Lockheed Martin Advanced Technology Center Palo Alto, CA, USA and the Polar/TIMAS,
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.
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.
Phase Coherence on Open Field Lines Associated with FLRs Abiyu Nedie, Frances Fenrich & Robert Rankin University of Alberta Edmonton, Alberta, Canada 2011.
Storm-Time Dynamics of the Inner Magnetosphere: Observations of Sources and Transport Michelle F. Thomsen Los Alamos National Laboratory 27 June 2003.
ULF Wave Modelling With A Motive: Effects on Energetic Paritcles Mary Hudson, Scot Elkington, Brian Kress, Kara Perry, John Lyon, Mike Wiltberger.
CISM Radiation Belt Models CMIT Mary Hudson CISM Seminar Nov 06.
Stanford Wave Induced Particle Precipitation (WIPP) Code Prajwal Kulkarni U.S. Inan, T.F. Bell March 4, 2008 Space, Telecommunications and Radioscience.
Radiation Belt Electron Transport & Energization inner belt outer belt Slot region Mary K. Hudson, Magnetospheric Thrust Participants.
CISM Advisory Council Meeting 4 March 2003 Magnetospheric Modeling Mary K. Hudson and the CISM Magnetospheric Modeling Team.
ULF Energy Transport Induced by Magnetospheric Boundary Oscillations Bill Lotko and Jeff Proehl Thayer School of Engineering Dartmouth College Boundary.
Magnetospheric Cavity Modes Driven by Solar Wind Dynamic Pressure Fluctuations: Initial results from LFM simulations Seth G. Claudepierre (Dartmouth College)
Finite Temperature Effects on VLF-Induced Precipitation Praj Kulkarni, U.S. Inan and T. F. Bell MURI Review February 18, 2009.
Magnetospheric Morphology Prepared by Prajwal Kulkarni and Naoshin Haque Stanford University, Stanford, CA IHY Workshop on Advancing VLF through the Global.
Observation and Theory of Substorm Onset C. Z. (Frank) Cheng (1,2), T. F. Chang (2), Sorin Zaharia (3), N. N. Gorelenkov (4) (1)Plasma and Space Science.
1 Dynamic Motion of Bow Shock and Magnetopause Observed by THEMIS Hui Zhang (BU) Q.-G. Zong (Umass Lowell) D. G. Sibeck (GSFC) T. A. Fritz (BU)
Overview of CISM Magnetosphere Research Mary Hudson 1, Anthony Chan 2, Scot Elkington 3, Brian Kress 1, William Lotko 1, Paul Melanson 1, David Murr 1,
Science Questions What is responsible for the "near" prompt onset of convection in the inner magnetosphere? Fast mode rarefraction wave?. How is the dayside.
RBSP observations: Poloidal ULF waves and drift-resonance wave particle interaction Lei Dai, Kazue Takahashi, John Wygant, EFW team. EMFISIS and ECT(MagEIS)
Stormtime plasmasheet access to the inner magnetosphere: evidence for an internal source S. R. Elkington LASP, University of Colorado, Boulder A. A. Chan,
Tuija I. Pulkkinen Finnish Meteorological Institute Helsinki, Finland
D. Sibeck, R. Millan, H. Spence
Combined Effects of Concurrent Pc5 and Chorus Waves on Relativistic Electron Dynamics Christos Katsavrias 1,2, Ioannis A. Daglis 2,1, Wen Li 3, Stavros.
Does Fermi Acceleration of account for variations of the fluxes of radiation belt particles observations at low altitudes during geomagnetic storms? J.
Comparisons of Inner Radiation Belt Formation in Planetary Magnetospheres Richard B Horne British Antarctic Survey Cambridge Invited.
Observation of Prompt Energization to ultra relativistic energies by the March 2015 interplanetary shock Shri Kanekal, Dan Baker, Bern Blake, Sam Califf,
1 Acceleration and Deceleration of Flare/Coronal Mass Ejection Induced Shocks S.T. Wu 1, C.-C. Wu 2, Aihua Wang 1, and K. Liou 3 1 CSPAR, University of.
Radiation Belts St. Petersburg (RBSPb) Meeting: List of Interesting Storms and Events Drew L. Turner and Mike Hartinger Mini-GEM: Dec
Drift Resonant Interactions of Radiation Belt Electrons with ULF waves. L. G. Ozeke, I. R. Mann, A. Degeling, V. Amalraj, and I. J. Rae University of Alberta.
Coupling of the Magnetosphere and Ionosphere by Alfvén Waves at High and Mid-Latitudes Bob Lysak, Yan Song, University of Minnesota, MN, USA Murray Sciffer,
Effective drift velocity and initiation times of interplanetary type-III radio bursts Dennis K. Haggerty and Edmond C. Roelof The Johns Hopkins University.
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.
Observation of high kinetic energy density jets in the Earth’s magnetosheath E. Amata 1, S. P. Savin 2, R. Treuman 3, G. Consolini 1, D. Ambrosino, M.F.
The Geoeffectiveness of Solar Cycle 23 as inferred from a Physics-Based Storm Model LWS Grant NAG Principal Investigator: Vania K. Jordanova Institute.
WG2 Summary Broke into ring current/plasmasphere and radiation-belt subgroups RING CURRENT Identified events for addressing science questions What is the.
17th Cluster workshop Uppsala, Sweden , May 12-15, 2009
1 ESS200C Pulsations and Waves Lecture Magnetic Pulsations The field lines of the Earth vibrate at different frequencies. The energy for these vibrations.
Multi-Spacecraft Observation of Compressional Mode ULF Waves Excitation and Relativistic Electron Acceleration X. Shao 1, L. C. Tan 1, A. S. Sharma 1,
Shock heating by Fast/Slow MHD waves along plasma loops
Van Allen Probes Extended Mission Science Theme (See next 3 slides for full articulations) 1.Structure of injections and shock-driven fronts. –Discussion.
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.
Storm-dependent Radiation Belt Dynamics Mei-Ching Fok NASA Goddard Space Flight Center, USA Richard Horne, Nigel Meredith, Sarah Glauert British Antarctic.
TRAD, Tests & Radiations ESWW11-session 5, November 18, 2014 Processing of the ACE/SIS heavy ion data in the frame of the ESA ESHIEM project Athina Varotsou.
Richard Thorne / UCLA Physical Processes Responsible for Relativistic Electron Variability in the Outer Radiation Zone over the Solar Cycle 1 Outline 2.
Earth’s Magnetosphere Space Weather Training Kennedy Space Center Space Weather Research Center.
Modelling Electron Radiation Belt Variations During Geomagnetic Storms with the new BAS Global Radiation Belt Model Richard B. Horne Sarah A. Glauert Nigel.
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.
Spacecast Richard B Horne, S. A. Glauert, N. P. Meredith, D. Boscher, V. Maget, A. Sicard, D. Heynderickx and D. Pitchford Forecasting the High Energy.
Modulation of chorus wave intensity by ULF waves from Van Allen Probes Observation Lunjin Chen 1, Zhiyang Xia 1, Lei Dai 2 1 Physics Dept., The University.
Plasma Wave Excitation Regions in the Earth’s Global Magnetosphere
Y. C.-M. Liu, M. Opher, O. Cohen P.C.Liewer and T.I.Gombosi
ARTEMIS – solar wind/ shocks
Suprathermal Particle Density Variations over the Solar Cycle
D.N. Baker, S. Kanekal, X. Li, S. Elkington
Acceleration and loss of relativistic and ultra-relativistic electrons in the outer Van Allen belt during intense storms: a statistical study. Christos.
A Pulsational Mechanism for Producing Keplerian Disks around Rapidly Rotating Stars Steven R. Cranmer Harvard-Smithsonian CfA.
Foster et al, jgr sub LFM-simulated shock arrival;
Geoffrey Reeves LANL.gov NewMexicoConsortium.org
Richard B. Horne British Antarctic Survey Cambridge UK
Presentation transcript:

October CME Shock Event Hudson, Paral, Kress, Turner SWE ACE Solar Wind Electron Proton Alpha Monitor K0>5-Min UT 8 Oct - 12UT 9 Oct 2013 n~ 55/cc v~660 km/s Replaced by ARTEMIS data – courtesy Drew Turner to fill data gap with higher time resolution for LFM-RCM simulations (6 sec input)

LFM-RCM Simulated M’pause Compression ARTEMIS solar wind inputACE solar wind input solar Mar ‘13 09 Oct ‘13

LFM-RCM Simulated Ephi along track of RBSP/A&B Oct 8 ‘13

LFM-RCM Simulated Ephi along track of RBSP/A&B Oct 8 ‘13 RBSP/B (blue) leads RBSP/A (red)

EFW data – FFT power at B (near apogee) at lower frequency than A at 2130 (green); A has moved to apogee by 2253 (aqua) - peak power shifts to lower frequency- FLR More power, lower f near apogee a) b)c) a) – c) refer to animation snapshots, next slide

Equatorial plane animation of E_phi showing m=2 mode structure; persistent E_phi<0=westward following shock accelerates electrons a) b) c) Shock arrival a); Propagates nightside b); Drop in Psw causes m’pause expansion c) reverse Ephi from a)

Equatorial plane animation of E_phi showing m=2 mode structure; persistent E_phi<0=west accel el

LFM-RCM ULF wave power, ARTEMIS input  Simulated m’pause 

8 Oct 1317 Mar 13 Simulated Magnetopause Shadowing Loss for 17 March and 8 Oct

Conclusions to Date for 8 Oct 13 E_phi ~ 10 mV/m common with CME shocks Energetic source population in outer zone is critical for significant drift resonant transport to produce new belts: electron v_phi ~ V_alfven req 8 Oct 2013 had both: source pop & Ephi 10mV/m Not a large Ephi event, persistent ULF oscillations: Comparable: 17 March 2013 simulations~10 mV/m ULF wave mode structure consistent with FLRs: Lower f at higher L favors drift resonance w/lower energy electrons at higher L, remaining drift res with higher f modes as they are transported inward; inward m’pause motion causes flux dropout at high L as obs Reference: Hudson et al., GRL, 2014 for Sept-Oct 2012 dropout simulations; GEM RBW focus group presentation - Mon 6/16 for 17 March & 8 Oct 13 results

Extra Slides Comparison of 17 March ’13 with 8 Oct ’12 ULF wave power, see Hudson et al., GRL, 2014

ULF Wave Power Comparison 17 March & 8 October ‘13 17 March 138 Oct 12