What DMSP Data Tell us About the Thermosphere Response to Solar Wind Forcing Delores Knipp CU Aerospace Engineering Sciences and NCAR HAO With Assistance.

Slides:



Advertisements
Similar presentations
SuperDARN is a network of HF radars (8-20 MHz) used to study the convection in the Earth's ionosphere at altitudes between 90 and 400 km and at magnetic.
Advertisements

Madeline Hubbard (Keene High School) Matthew Shindel (Stanwich High School) Advisors: Fathima Muzamil, Dr. Charles Farrugia, Dr. Roy Torbert Objective:
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.
On the Generation of Enhanced Sunward Convection and Transpolar Aurora in the High- Latitude Ionosphere by Magnetic Merging S. Eriksson 1, J. B. H. Baker.
Generation of the transpolar potential Ramon E. Lopez Dept. of Physics UT Arlington.
Anti-Parallel Merging and Component Reconnection: Role in Magnetospheric Dynamics M.M Kuznetsova, M. Hesse, L. Rastaetter NASA/GSFC T. I. Gombosi University.
Principles of Global Modeling Paul Song Department of Physics, and Center for Atmospheric Research, University of Massachusetts Lowell Introduction Principles.
Cluster, THEMIS, & Geotail Conjunction Event on 11 July 2008 Hiroshi Hasegawa ISAS/JAXA.
Formation of the Magnetosphere 1 Solar Wind. Formation of the Magnetosphere 2 Solar Wind Bow Shock Magnetosheath.
ESS 7 Lecture 14 October 31, 2008 Magnetic Storms
The role of solar wind energy flux for transpolar arc luminosity A.Kullen 1, J. A. Cumnock 2,3, and T. Karlsson 2 1 Swedish Institute of Space Physics,
IMF Bx influence on the magnetotail neutral sheet geometry and dynamics E. Gordeev, M. Amosova, V. Sergeev Saint-Petersburg State University, St.Petersburg,
Spatial distribution of the auroral precipitation zones during storms connected with magnetic clouds O.I. Yagodkina 1, I.V. Despirak 1, V. Guineva 2 1.
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,
Occurrence and properties of substorms associated with pseudobreakups Anita Kullen Space & Plasma Physics, EES.
Plasma entry in the Mercury’s magnetosphere S. Massetti S. Massetti INAF-IFSI Interplanetary Space Physics Institute, Roma - Italy.
Solar wind-magnetosphere coupling Magnetic reconnection In most solar system environments magnetic fields are “frozen” to the plasma - different plasmas.
Observation of Auroral-like Peaked Electron Distributions at Mars D.A. Brain, J.S. Halekas, M.O. Fillingim, R.J. Lillis, L.M. Peticolas, R.P. Lin, J.G.
Origin of Ionospheric Hot Spots During Quiet Times J. Raeder, W. Li Space Science Center, UNH D. Knipp NCAR/HAO MURI/NADIR Workshop, Boulder, CO, October.
OpenGGCM Simulation vs THEMIS Observations in an Dayside Event Wenhui Li and Joachim Raeder University of New Hampshire Marit Øieroset University of California,
State Key Laboratory of Space Weather An inter-hemisphere asymmetry of the cusp region against the geomagnetic dipole tilt Jiankui Shi Center for Space.
O. M. Shalabiea Department of Physics, Northern Borders University, KSA.
Reinisch_ Solar Terrestrial Relations (Cravens, Physics of Solar Systems Plasmas, Cambridge U.P.) Lecture 1- Space Environment –Matter in.
& Atmospheric StudiesPhysics & Engineering Physics, University of Saskatchewan Hemispheric Comparison of Signatures of.
Location of the High-Latitude Reconnection Site on 14 February 2003 S. Eriksson 1, M. M. Kuznetsova 2, M. W. Dunlop 3, and H. Reme 4 1 LASP, University.
FA III – High Latitude Energy Partitioning and Density Implications Jeff Thayer University of Colorado Team: Mihail Codrescu, Geoff Crowley, Jeff Forbes,
Ionospheric Convection Response to High-Latitude Reconnection and Electrodynamics of a Split-Transpolar Aurora S. Eriksson 1, G. Provan 2, F. J. Rich 3,
Thermospheric Density Enhancements from Unexpected Energy Deposition During Bz North and Strong By Conditions Geoff Crowley, ASTRA Delores Knipp, NCAR.
Importance of the Height Distribution of Joule Heating for Thermospheric Density Arthur D. Richmond and Astrid Maute NCAR High Altitude Observatory.
MAGNETOTAIL LOBE POPULATION AS MEASURED BY INTERBALL-1 SATELLITE Koleva R. 1, Grigorenko E. 2, Sauvaud J.-A. 3 (1) Solar-Terrestrial Influences Laboratory,
Location of Magnetopause Reconnection S M Petrinec 1, S A Fuselier 1, K J Trattner 1, and J Berchem 2 1 Lockheed Martin Advanced Technology Center, Palo.
Figure 1: show a causal chain for how Joule heating occurs in the earth’s ionosphere Figure 5: Is of the same format as figure four but the left panels.
1 Cambridge 2004 Wolfgang Baumjohann IWF/ÖAW Graz, Austria With help from: R. Nakamura, A. Runov, Y. Asano & V.A. Sergeev Magnetotail Transport and Substorms.
How does the Sun drive the dynamics of Earth’s thermosphere and ionosphere Wenbin Wang, Alan Burns, Liying Qian and Stan Solomon High Altitude Observatory.
University of Colorado 1 ; Delft University of Technology 2 ; University of Alaska 3 ; Centre National d’Etudes Spatiales 4 ; National Center for Atmospheric.
Space Weather: Magnetic Storms 31 October 2011 William J. Burke Air Force Research Laboratory/Space Vehicles Directorate Boston College Institute for Scientific.
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.
Localized Thermospheric Energy Deposition Observed by DMSP Spacecraft D. J. Knipp 1,2, 1 Unversity of Colorado, Boulder, CO, USA 2 High Altitude Observatory,
PAPER I. ENA DATA ANALYSIS RESULTS. The Imager for Magnetopause-to- Aurora Global Exploration (IMAGE) missionis the first NASA Mid-size Explorer (MIDEX)
Earth’s Magnetosphere — A very quick introduction Weichao Tu - LASP of CU-Boulder CEDAR-GEM Joint Workshop - Santa Fe, NM - 06/26/2011.
Large electric fields near the nightside plasmapause observed by the Polar spacecraft K.-H. Kim 1, F. Mozer 2, and D.-H. Lee 1 1 Department of Astronomy.
Response of the Magnetosphere and Ionosphere to Solar Wind Dynamic Pressure Pulse KYUNG SUN PARK 1, TATSUKI OGINO 2, and DAE-YOUNG LEE 3 1 School of Space.
Intense Poynting flux at very high latitudes during magnetic storms: GITM simulation results Yue Deng 1 Cheng Sheng 1, Manqi Shi 1, Yanshi Huang 2, Cheryl.
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.
Simultaneous in-situ observations of the feature of a typical FTE by Cluster and TC1 Zhang Qinghe Liu Ruiyuan Polar Research Institute of China
PARTICLES IN THE MAGNETOSPHERE
Mass Transport: To the Plasma Sheet – and Beyond!
Publications in Comparative Magnetospheres Siscoe, G. L.: Towards a comparative theory of magnetospheres, in Solar System Plasma Physics, Vol. II, edited.
Global MHD Simulation with BATSRUS from CCMC ESS 265 UCLA1 (Yasong Ge, Megan Cartwright, Jared Leisner, and Xianzhe Jia)
NASA NAG Structure and Dynamics of the Near Earth Large-Scale Electric Field During Major Geomagnetic Storms P-I John R. Wygant Assoc. Professor.
Magnetic reconnection in the magnetotail: Geotail observations T. Nagai Tokyo Institute of Technology World Space Environment Forum 2005 May 4, 2005 Wednesday.
Study on the Impact of Combined Magnetic and Electric Field Analysis and of Ocean Circulation Effects on Swarm Mission Performance by S. Vennerstrom, E.
Stuart D. BaleFIELDS SOC CDR – Science Requirements Solar Probe Plus FIELDS SOC CDR Science and Instrument Overview Science Requirements Stuart D. Bale.
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.
Particle precipitation has been intensely studied by ionospheric and magnetospheric physicists. As particles bounce along the earth's magnetic fields they.
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.
Energy inputs from Magnetosphere to the Ionosphere/Thermosphere ASP research review Yue Deng April 12 nd, 2007.
Magnetotail Reconnection T. Nagai Tokyo Institute of Technology Harry Petschek Symposium on Magnetic Reconnection March 22, 2006 Wednesday 12:00 – 12:30.
Cluster observation of electron acceleration by ULF Alfvén waves
Challenges The topological status of the magnetosphere: open or closed? Driver(s) of ionospheric sunward flow Source(s) of NBZ currents Key problem: are.
Paul Song Center for Atmospheric Research
High-latitude Neutral Density Maxima
Global MHD Simulations of Dayside Magnetopause Dynamics.
Evidence for Dayside Interhemispheric Field-Aligned Currents During Strong IMF By Conditions Seen by SuperDARN Radars Joseph B.H. Baker, Bharat Kunduri.
The Physics of Space Plasmas
Principles of Global Modeling
Solar Wind-Magnetosphere Interaction: Reconnection and IMF Dependence
Magnetosphere: Bow Shock Substorm and Storm
Presentation transcript:

What DMSP Data Tell us About the Thermosphere Response to Solar Wind Forcing Delores Knipp CU Aerospace Engineering Sciences and NCAR HAO With Assistance from Liam Kilcommons, CSU

What DMSP Data Tell us About the Thermosphere Response to Solar Wind Forcing - Energy deposition on the dayside can be strongly controlled by the IMF By component -Even during strong storms energy deposition on the dayside may exceed that on the nightside -Orbit Integrated Poynting flux (and DMSP  B) show the physical link between solar wind and neutral density periodicities - During strong IMF By events magnetosheath particles are supplementing the energy deposition by Poynting flux…..but at a different altitude - During high speed streams energy deposition on the dayside dominates that on the nightside

Adapted from Day, C., Spacecraft probes the site of magnetic reconnection in Earth's magnetotail, Physics Today, Vol. 54, No. 10, 16-17, Adapted from NASA Press release: Connection of Sun's and Earth's magnetic fields provides energy for auroras, space weather, Southward IMFNorthward IMF Schematics of magnetopause reconnection for IMF Bz illustrating the topological differences in reconnection location, depending upon the interplanetary magnetic field direction.

Park et al., 2006 Merging location simulation with dipole tilt of 30, IMF Bz = –5 nT, and IMF By = 5 nT

When IMF Bz is negative and By is present Merged flux tubes are accelerated azimuthally, Dayside flow channel s develop between convections cells R1 field aligned currents become asymmetric near noon – Negative (dawnward) west, Those connected to the southern (northern) hemisphere move duskward (dawnward) Downward R1 currents dominate the noon sector in the northern hemisphere - Positive (duskward) east, Those connected to the southern (northern) hemisphere move dawnward (duskward) Upward R1 currents dominate the noon sector in the northern hemisphere N N (Weimer, 2005 and Anderson, et al. 2008)

When IMF Bz is positive and By is present Merged flux tubes are accelerated azimuthally, Dayside flow channel s develop but appear to be more variable R1 field aligned currents become asymmetric near noon, R0 field aligned currents may be present Strong IMF and high speed flow may provide more clarity (Weimer, 2005 and Anderson, et al. 2008)

Poynting Vector from Defense Meteorological Satellite Program S/C DMSP instruments sense Electric and Magnetic Fields Y X Z Spacecraft track

Cusp reconnection near the dawn flank Field lines map across dayside Near-Cusp energy source during strong IMF By: Li et al. Southern lobe field lines Obs DMSP Mag Perturbations Calculated DMSP Poynting Flux OPENGGCM Joule Heating SH SH B z ~+10nT B Y ~+25nT V SW ~ 950 km/s OPENGGCM FAC

Poynting Flux Delta BxDelta By Vy DMSP Data and Calculations

Aug Large IMF By, Bz~0 Neutral Density Crowley et al., 2010

Poynting FluxParticle Flux Vz DMSP Data and Calculations ….not quite the full story…..

High-Latitude Energy Input: Field and Particles Poynting FluxParticle Flux

Poynting FluxParticle Flux Vz DMSP Data and Calculations ….not quite the full story…..

2005 Poynting Flux and Solar Wind Speed Lomb-Scargle Periodogram

DMSP F-15 Orbit Integrated |dB y | for 2005 Blue = angles in the range , typical away or positive polarity. Red denotes angles in the range ., typical toward or negative polarity. Yellow denotes angles in either of the other two azimuthal quadrants. Orbit Integrated dBy

DMSP F-15 Orbit Integrated dB y for 2005 Blue = angles in the range , typical away or positive polarity. Red denotes angles in the range ., typical toward or negative polarity. Yellow denotes angles in either of the other two azimuthal quadrants. Orbit Integrated dBy

Intense Magnetic Storm Jan

High-speed Stream August

AMIE Joule Heating and Electric Potential During High Speed Flow 00 UT 16 Aug 2005 Courtesy of G. Crowley

AMIE Joule Heating and Electric Potential During High Speed Flow 04 UT 16 Aug 2005 Courtesy of G. Crowley

AMIE Joule Heating and Electric Potential During High Speed Flow 1040 UT 16 Aug 2005 Courtesy of G. Crowley

AMIE Joule Heating and Electric Potential During High Speed Flow 2045 UT 16 Aug 2005 Courtesy of G. Crowley

What DMSP Data Tell us About the Thermosphere Response to Solar Wind Forcing - Energy deposition on the dayside is strongly controlled by the IMF By component -Even during strong storms energy deposition on the dayside may exceed that on the nightside -Orbit Integrated Poynting flux (and DMSP  B) show the physical link between solar wind and neutral density periodicities - During strong IMF By events magnetosheath particles are supplementing the energy deposition by Poynting flux…..but at a different altitude - During high speed streams energy deposition on the dayside dominates that on the nightside