Observations of reflected ions downstream of shocks in the heliosphere John Richardson M.I.T. (Voyager plasma experiment) 10 – 5950 eV/q.

Slides:



Advertisements
Similar presentations
Heavy Ion Abundances in Large Solar Energetic Particle Events Spring AGU 2006, SH43B-04 Heavy Ion Abundances in Large Solar Energetic Particle Events Spring.
Advertisements

Plasma-induced Sputtering & Heating of Titan’s Atmosphere R. E. Johnson & O.J. Tucker Goal Understand role of the plasma in the evolution of Titan’s atmosphere.
The Johns Hopkins University Applied Physics Laboratory SHINE 2005, July 11-15, 2005 Transient Shocks and Associated Energetic Particle Events Observed.
On the link between the solar energetic particles and eruptive coronal phenomena On the link between the solar energetic particles and eruptive coronal.
Foreshock studies by MEX and VEX FAB: field-aligned beam FAB + FS: foreshock M. Yamauchi et al.
Session A Wrap Up. He Abundance J. Kasper Helium abundance variation over the solar cycle, latitude and with solar wind speed Slow solar wind appears.
A Whole-Heliosphere View of the Solar Wind Hale Lecture American Astronomical Society 5/24/2010 Marcia Neugebauer University of Arizona.
ESS 7 Lecture 14 October 31, 2008 Magnetic Storms
Low-Frequency Waves Excited by Newborn Interstellar Pickup Ions H + and He + at 4.5 AU Charles W. Smith, Colin J. Joyce, Philip A. Isenberg, Neil Murphy,
Inner Source Pickup Ions Pran Mukherjee. Outline Introduction Current theories and work Addition of new velocity components Summary Questions.
Observations of Pickup Ions and their Tails in the Heliosphere and Heliosheath George Gloeckler University of Michigan, Ann Arbor, MI Implications of Interstellar.
Comparing the solar wind-magnetosphere interaction at Mercury and Saturn A. Masters Institute of Space and Astronautical Science, Japan Aerospace Exploration.
1 Diagnostics of Solar Wind Processes Using the Total Perpendicular Pressure Lan Jian, C. T. Russell, and J. T. Gosling How does the magnetic structure.
The Acceleration of Anomalous Cosmic Rays by the Heliospheric Termination Shock J. A. le Roux, V. Florinski, N. V. Pogorelov, & G. P. Zank Dept. of Physics.
CME Workshop Elmau, Feb , WORKING GROUP C: ENERGETIC PARTICLE OBSERVATIONS Co-Chairs: Klecker, Kunow SUMMARY FROM WORKSHOP 1 Observations Questions.
STEREO AND SPACE WEATHER Variable conditions in space that can have adverse effects on human life and society Space Weather: Variable conditions in space.
Solar wind interaction with the comet Halley and Venus
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)
C. May 12, 1997 Interplanetary Event. Ambient Solar Wind Models SAIC 3-D MHD steady state coronal model based on photospheric field maps CU/CIRES-NOAA/SEC.
Solar system science using X-Rays Magnetosheath dynamics Shock – shock interactions Auroral X-ray emissions Solar X-rays Comets Other planets Not discussed.
Plasma in the Heliosheath John Richardson M.I.T. Collaborators: J. Belcher, J. Kasper, E. Stone, C. Wang.
Interstellar and Interplanetary Material HST Astrobiology Workshop: May 5-9, 2002 P.C. Frisch University of Chicago.
The Injection Problem in Shock Acceleration The origin of the high-energy cosmic rays remains one of the most-important unsolved problems in astrophysics.
November 2006 MERCURY OBSERVATIONS - JUNE 2006 DATA REVIEW MEETING Review of Physical Processes and Modeling Approaches "A summary of uncertain/debated.
Benoit Lavraud CESR/CNRS, Toulouse, France Uppsala, May 2008 The altered solar wind – magnetosphere interaction at low Mach numbers: Magnetosheath and.
Ion dynamics and shock front nonstationarity in supercritical perpendicular shocks: impact of the pickup ions Zhongwei YANG 1 and Quanming LU 2 1 SOA Key.
Solar Modulation: A Theoretical Perspective Modeling of cosmic ray charge-sign dependence in the heliosphere Marius Potgieter Unit for Space Physics North-West.
1 Origin of Ion Cyclotron Waves in the Polar Cusp: Insights from Comparative Planetology Discovery by OGO-5 Ion cyclotron waves in other planetary magnetospheres.
Space Weather from Coronal Holes and High Speed Streams M. Leila Mays (NASA/GSFC and CUA) SW REDISW REDI 2014 June 2-13.
14 May JIM M. RAINES University of Michigan DANIEL J. GERSHMAN, THOMAS H. ZURBUCHEN, JAMES A. SLAVIN, HAJE KORTH, and BRIAN J. ANDERSON Magnetospheric.
Observational Tests of Suprathermal Particle Acceleration (Dayeh/Hill  Hill/Desai) WORKING GROUP SUMMARY.
The Solar System Journey to Outer Space. Overview  The Solar System includes:  The sun  The eight official planets  At least three draft planets 
Solar Wind and Coronal Mass Ejections
1 N. A. Schwadron - Hawaii -2009Interstellar Interaction Observed Jan 7, 2009 The Interstellar Interaction Observed N. A. Schwadron, J. Richardson, P.
1 SEP “Campaign Events” for SHINE 2003 Question: Can we identify solar/interplanetary factors that drive SEP spectral and compositional variability at.
ASEN5335- Aerospace Environments -- The Solar Wind 1 THE INTERPLANETARY MEDIUM AND IMF Consequently, the "spiral" pattern formed by particles spewing.
Pre-accelerated seed populations of energetic particles in the heliosphere N. A. Schwadron* and M. Desai Southwest Research Institute *Also, Boston University.
SHINE 2006 Student Day Working Group III summary Zermatt, Utah, July 31 - August 4 Gang Li.
1 Hybrid Simulations of the Callisto - Magnetosphere Interaction Stas Barabash and Mats Holmström Swedish Institute of Space Physics, Kiruna, Sweden.
Outline ■The Heliosphere, Astrospheres and the Interstellar Interaction ● Implications of Recent Voyager Results ■Energetic Neutral Atoms [ENAs], ENA Imaging.
Quo vadis? Jeffrey Hughes Boston University. Quo vadis? Where are you going?
A shock is a discontinuity separating two different regimes in a continuous media. –Shocks form when velocities exceed the signal speed in the medium.
The Suprathermal Tail Properties are not well understood; known contributors Heated solar wind Interstellar and inner source pickup ions Prior solar and.
Solar Energetic Particles (SEP’s) J. R. Jokipii LPL, University of Arizona Lecture 2.
Introduction to Space Weather Jie Zhang CSI 662 / PHYS 660 Fall, 2009 Copyright © The Heliosphere: Solar Wind Oct. 08, 2009.
Nature, Distribution and Evolution of Solar Wind Turbulence throughout the Heliosphere W. H. Matthaeus Bartol Research Institute, University of Delaware.
08/4/2009NAS - SHINE-Suprathermal Radial Evolution (1-11 AU) of Pickup Ions and Suprathermal Ions in the Heliosphere N. A. Schwadron Boston University,
ASEN 5335 Aerospace Environments -- Magnetospheres 1 As the magnetized solar wind flows past the Earth, the plasma interacts with Earth’s magnetic field.
1 N. A. Schwadron - NESSC -2009Interstellar Interaction Observed Jan 7, 2009 The Interstellar Interaction Observed N. A. Schwadron on behalf of the IBEX.
Low-energy Ion Distributions at the Termination Shock Rob Decker Johns Hopkins Univ., Applied Physics Lab., Laurel, MD SHINE, June-2008, Zermatt.
CLICK TO CONTINUE CLICK TO CONTINUE. The Sun Inner Solar System Inner Solar System Outer Solar System Outer Solar System.
IPS tomography IPS-MHD tomography. Since Hewish et al. reported the discovery of the interplanetary scintillation (IPS) phenomena in 1964, the IPS method.
1. What controls the occurrence of reconnection. 2
Nature, Distribution and Evolution of Solar Wind Turbulence throughout the Heliosphere W. H. Matthaeus Bartol Research Institute, University of Delaware.
George C. Ho1, David Lario1, Robert B. Decker1, Mihir I. Desai2,
Progress Toward Measurements of Suprathermal Proton Seed Particle Populations J. Raymond, J. Kohl, A. Panasyuk, L. Gardner, and S. Cranmer Harvard-Smithsonian.
Introduction to Space Weather Interplanetary Transients
Voyager Observations in the Heliosheath: An Overview
Student Day Working Group III summary
Solar Wind Transients and SEPs
The limits of the solar system
M. Yamauchi1, Y. Futaana1, R. Lundin1, S. Barabash1, M. Wieser1, A
The Bow Shock and Magnetosheath
Introduction to Space Weather
Physics 320: Interplanetary Space and the Heliosphere (Lecture 24)
solar wind – bow shock - magnetosheath
International Workshop

The Solar System.
Presentation transcript:

Observations of reflected ions downstream of shocks in the heliosphere John Richardson M.I.T. (Voyager plasma experiment) 10 – 5950 eV/q

Sheaths and Scales 100s AU AU ~R S - 10s AU

Outline A) Reflected ions: 1.Earth 2.Outer planets 3.Termination Shock 4.Interplanetary shocks B) Shocks in local interstellar medium? Shakespeare?

Sir Isaac Newton: The Principia: Book 3, De mundi systemate

Reflected ions: In high Mach number shocks energy is dissipated via reflected ions. Some thermal ions are reflected by the shock potential at their first shock encounter and gain additional energy. (Fuselier and Schmidt, 1994)

Ratio of reflected to total ion density: Observations, simulation, and theory Ratio increases with Mach number to plateau at about 20-25% T(ref)/T(th) = 3-5 (Fuselier and Schmidt, 1994). Earth’s bow shock

Ion Distributions Ion distributions, Jovian magnetosheath Fit with 2 isotropic Maxwellian proton components. V(R,T,N) = (114, 87, 1) km/s, N=(.68,.79) cm-3, T=(100, 598) eV 54% reflected; T(ref)/T(th)= eV 6 keV

Outer Planets Jupiter Saturn Uranus Neptune N H /N T T H /T C T 5.1e6 4.8e6 2.6e6 3.6e6 Comparison of Reflected Ions Jupiter % reflected ions and T H /T C increase with distance (with exception of Uranus).  >25%, not consistent with theory.  70-85% of energy in reflected ions

Downstream of termination shock No reflected ions observed in HSH T ~ 150,000 K V > Wth Most of SW energy goes into pickup ions, some of which are reflected. (Zank et al., 1996)

Interstellar neutrals dominate density outside ~10 AU Pickup ions dominate thermal pressure outside 30 AU First effects of LIC on solar wind are from these neutrals.

Energy/proton |B| Energy/proton decreases before and at TS: shock mediated by energetic particles (Florinski et al.). ~20 % of flow energy to thermal plasma: rest to pickup ions and energetic particles.

Interplanetary Shocks: Select largest (CME driven, mainly MIRs)

% of Reflected ions vs. distance: IP shocks and bow shocks FF (IP) and FR (BS and TS) shocks 35

T(ref)/T(th) vs. distance: IP shocks and bow shocks

Jupiter Saturn Uranus Neptune ICME TS N H /N T T H /T C T 5.1e6 4.8e6 2.6e6 3.6e e5 Uranus has H corona - perhaps creates own pickup ions? Comparison of Reflected Ions Jupiter ICME Termination shock

Summary Reflected ions increase with distance to ~35 AU, then disappear. Pickup ions gain most of flow energy after 35 AU Weak shock-like structures observed in LISM with very large widths.