Finding the Source of Ion Beams in the Solar Wind Hanna Kristensen Advisors: Justin Kasper and Mike Stevens.

Slides:



Advertisements
Similar presentations
Multiple reconnections and explosive events and in MST and solar flares Gennady Fiksel CMSO workshop, Princeton, NJ, Oct 5-8, 2005.
Advertisements

Anomalous Ion Heating Status and Research Plan
The Johns Hopkins University Applied Physics Laboratory SHINE 2005, July 11-15, 2005 Transient Shocks and Associated Energetic Particle Events Observed.
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.
Momentum Transport During Reconnection Events in the MST Reversed Field Pinch Alexey Kuritsyn In collaboration with A.F. Almagri, D.L. Brower, W.X. Ding,
Ion Pickup One of the fundamental processes in space plasma physics.
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.
Temporal Separation of AIA 131 Å and GOES 1-8 Å Peak Flux in Solar Flares Daniel Herman Reed College ‘15 Advisors: Dr. Kathy Reeves & Dr. Trae Winter 8/14/2014.
Alfvén-cyclotron wave mode structure: linear and nonlinear behavior J. A. Araneda 1, H. Astudillo 1, and E. Marsch 2 1 Departamento de Física, Universidad.
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.
Modeling the Neupert Effect in Flares: Connecting Theory and Observation Andrea Egan Advisors: Dr. Trae Winter and Dr. Kathy Reeves.
Further Study of Ion Pickup. Turbulent Alfven waves and magnetic field lines Turbulent waves represent enhanced random fluctuations. Fluctuations vitiate.
Solar Flare Particle Heating via low-beta Reconnection Dietmar Krauss-Varban & Brian T. Welsch Space Sciences Laboratory UC Berkeley Reconnection Workshop.
Prob, % WinterSummer Probability of observing downward field-aligned electron energy flux >10 mW/m 2 in winter and summer hemispheres.
Carlson et al. ‘01 Three Characteristic Acceleration Regions.
Magnetic Reconnection in the Solar Wind Gosling, Phan, et al.
Evidence of Thick Reconnection Layers in Solar Flares John Raymond Work with A. Ciaravella, Y.-K. Ko and J. Lin White Light and UV Observations Apparent.
Winds of cool supergiant stars driven by Alfvén waves
In-situ Observations of Collisionless Reconnection in the Magnetosphere Tai Phan (UC Berkeley) 1.Basic signatures of reconnection 2.Topics: a.Bursty (explosive)
Progenitors to Geoeffective Coronal Mass Ejections: Filaments and Sigmoids David McKenzie, Robert Leamon Karen Wilson, Zhona Tang, Anthony Running Wolf.
Hybrid simulations of parallel and oblique electromagnetic alpha/proton instabilities in the solar wind Q. M. Lu School of Earth and Space Science, Univ.
On the Cause of Solar Differential Rotation Ling-Hsiao Lyu Institute of Space Science, National Central University 呂凌霄 中央大學太空科學研究所 太陽差動自轉的成因.
Dissipation of Alfvén Waves in Coronal Structures Coronal Heating Problem T corona ~10 6 K M.F. De Franceschis, F. Malara, P. Veltri Dipartimento di Fisica.
Asymmetric Magnetic Reconnection in Coronal Mass Ejection Current Sheets Crystal L. Pope Elmhurst College Advisors: Nick Murphy & Mari Paz Miralles Harvard-Smithsonian.
Plasma in the Heliosheath John Richardson M.I.T. Collaborators: J. Belcher, J. Kasper, E. Stone, C. Wang.
Magnetic Waves in Solar Coronal Loops Ryan Orvedahl Stony Brook University Advisor: Aad van Ballegooijen Center for Astrophysics.
Incorporating Kinetic Effects into Global Models of the Solar Wind Steven R. Cranmer Harvard-Smithsonian Center for Astrophysics.
Magnetic Reconnection in Multi-Fluid Plasmas Michael Shay – Univ. of Maryland.
MHD Modeling of the Large Scale Solar Corona & Progress Toward Coupling with the Heliospheric Model.
Measuring the Magnetic Field in the Sun and the Interstellar Medium Steven R. Spangler… University of Iowa.
Elements of kinetic theory Introduction Phase space density Equations of motion Average distribution function Boltzmann-Vlasov equation Velocity distribution.
Non-collisional ion heating and Magnetic Turbulence in MST Abdulgader Almagri On behalf of MST Team RFP Workshop Padova, Italy April 2010.
Accuracy of spacecraft measurements of solar wind plasma: Past, Present and Future John Podesta & John Steinberg Organizers Shine Workshop, July 6-10,
Physical analogies between solar chromosphere and earth’s ionosphere Hiroaki Isobe (Kyoto University) Acknowledgements: Y. Miyoshi, Y. Ogawa and participants.
Two-dimensional hybrid modeling of wave heating in the solar wind plasma L. Ofman 1, and A.F. Viñas 2 1 Department of Physics, Catholic University of America,
Coronal Heating of an Active Region Observed by XRT on May 5, 2010 A Look at Quasi-static vs Alfven Wave Heating of Coronal Loops Amanda Persichetti Aad.
Solar Physics & Space Plasma Research Center (SP 2 RC) The role of partial ionisation in the stability of prominences structures Istvan Ballai SP 2 RC,
The Sun and the Heliosphere: some basic concepts…
Numerical simulations are used to explore the interaction between solar coronal mass ejections (CMEs) and the structured, ambient global solar wind flow.
Probing Energy Release of Solar Flares M. Prijatelj Carnegie Mellon University Advisors: B. Chen, P. Jibben (SAO)
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.
The energetics of the slow solar wind Leon Ofman, Catholic University of America, NASA GSFC, Code 612.1, Greenbelt, MD 20771, USA
1 Searching for Alfvén Waves John Yoritomo The Catholic University of America Mentor: Dr. Adriaan van Ballegooijen The Smithsonian Astrophysical Observatory.
Why Solar Electron Beams Stop Producing Type III Radio Emission Hamish Reid, Eduard Kontar SUPA School of Physics and Astronomy University of Glasgow,
Cold plasma: a previously hidden solar system particle population Mats André and Chris Cully Swedish Institute of Space Physics, Uppsala.
Earth’s Magnetosphere NASA Goddard Space Flight Center
II. MAGNETOHYDRODYNAMICS (Space Climate School, Lapland, March, 2009) Eric Priest (St Andrews)
Spectroscopic Detection of Reconnection Evidence with Solar-B II. Signature of Flows in MHD simulation Hiroaki ISOBE P.F. Chen *, D. H. Brooks, D. Shiota,
Chapman Conference “Fundamental Properties and Processes of Magnetotails” 12 March 2013, Tuesday, p.m. Structure of Magnetic Reconnection in the.
Courtesy of John Kirk Particle Acceleration. Basic particle motion No current.
Simulation Study of Magnetic Reconnection in the Magnetotail and Solar Corona Zhi-Wei Ma Zhejiang University & Institute of Plasma Physics Beijing,
Simultaneous in-situ observations of the feature of a typical FTE by Cluster and TC1 Zhang Qinghe Liu Ruiyuan Polar Research Institute of China
ORIGIN OF THE SLOW SOLAR WIND K. Fujiki , T. Ohmi, M. Kojima, M. Tokumaru Solar-Terrestrial Environment Laboratory, Nagoya University and K. Hakamada Department.
1 ESS200C Pulsations and Waves Lecture Magnetic Pulsations The field lines of the Earth vibrate at different frequencies. The energy for these vibrations.
Magnetic reconnection in the magnetotail: Geotail observations T. Nagai Tokyo Institute of Technology World Space Environment Forum 2005 May 4, 2005 Wednesday.
Space physics EF2245 Tomas Karlsson Space and Plasma Physics School of Electrical Engineering EF2245 Space Physics 2010.
Stuart D. BaleFIELDS SOC CDR – Science Requirements Solar Probe Plus FIELDS SOC CDR Science and Instrument Overview Science Requirements Stuart D. Bale.
Shock heating by Fast/Slow MHD waves along plasma loops
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.
Multi-Fluid/Particle Treatment of Magnetospheric- Ionospheric Coupling During Substorms and Storms R. M. Winglee.
Generation of anomalously energetic suprathermal electrons by an electron beam interacting with a nonuniform plasma Dmytro Sydorenko University of Alberta,
Sweet Solar SAP: Boiling Down the Thermal Energy Content of Supra-Arcade Plasma Ashley Armstrong Advisor: Dr. Kathy Reeves Solar REU Summer 2012.
The heliospheric magnetic flux density through several solar cycles Géza Erdős (1) and André Balogh (2) (1) MTA Wigner FK RMI, Budapest, Hungary (2) Imperial.
Chapman Conference “Fundamental Properties and Processes of Magnetotails” 12 March 2013, Tuesday, p.m. Structure of Magnetic Reconnection in the.
Time-Dependence (structuring) of the Alpha-to-Proton Ratio (A He ) in the Solar Wind at 1 AU: Initial results, Implications, and Speculations Harlan E.
How does the solar atmosphere connect to the inner heliosphere?
Series of high-frequency slowly drifting structure mapping the magnetic field reconnection M. Karlicky, A&A, 2004, 417,325.
Heavy-Ion Acceleration and Self-Generated Waves in Coronal Shocks
Evidence for magnetic reconnection in the high corona
Generation of Alfven Waves by Magnetic Reconnection
Presentation transcript:

Finding the Source of Ion Beams in the Solar Wind Hanna Kristensen Advisors: Justin Kasper and Mike Stevens

Solar Wind Plasma frozen into magnetic field lines (by the Lorentz Force) The proton density, velocity, temperature vary – n~ a few cm -3 – v~ hundreds of km/s – w~ tens of km/s Usually not in thermodynamic equilibrium!

Maxwell distribution

Magnetic Reconnection

Reconnection Sites Gosling et al., 2005

Wind Faraday Cup Sitting at the first LaGrange point Spinning at 3 second period 2 Faraday cups (one tilted up and one down) SWE

Data Collection

March 25, :45 16:00 16:15 16:30 16:45 B y [nT] B z [nT] B x [nT] v y [km/s] v z [km/s] v x [km/s] (red points signify a beam detected)

Density in the exhaust

Transformation Out-of-plane speed [km/s] Inflow speed [km/s] Outflow speed [km/s]

Fits Ion Flux Distribution for March 25, 1998; 16:21

YearDayAlfvén Speed (km/s) Differential Speed ΔV (km/s) Inflow Speed (km/s)

Relationship between inflow speed and Δv

Differential flow vs. Alfvén speed

Plasma Instabilities

Instability Evolution Configurations with ∆v››v A are unstable! Beam loses energy to Alfvénic fluctuations Waves become stronger Waves scramble the structure Growth rate is faster than the time it takes plasma to cross the exhaust Yoshiharu Omura and Koichi Shin Research Institute for Sustainable Humanosphere, Kyoto University

Conclusions Beams do develop in magnetic reconnection exhausts Their speed actually exceeds the inflow speed – Acceleration process? In some cases, an unstable beam-core configuration arises (Alfvén/Ion cyclotron mode)

Acknowledgements Dr. Michael Stevens and Dr. Justin Kasper NSF (grant number AGS ) CFA Dr. Kathy Reeves and Dr. Trae Winter SSXG & Admins Fellow astronomy and solar interns

Questions What is the process that accelerates the beams faster than the inflow? How does the instability affect the evolution of reconnection exhausts

Much of the solar wind has Alfvénic beams of coronal origin This is the stuff we think reconnection might explain We actually found this stuff in some reconnection exhausts