Andrew W. Yau University of Calgary, Canada CASSIOPE Enhanced Polar Outflow Probe (e-POP) University of Alberta, October 25, 2007.

Slides:



Advertisements
Similar presentations
Abstract Real-time images of Earths space environment from NASAs IMAGE satellite will soon be available on the NOAA Space Environment Center Web site.
Advertisements

Space Weather dependence of the air drag as observed by CHAMP Hermann Lühr 1) and Huixin Liu 2) 1) GeoForschungsZentrum Potsdam, Germany 2) Dept. Earth.
1 Kuafu A mission to start a mission William Liu Canadian Space Agency & Chinese Academy of Sciences August 29, 2011, 3rd ILWS Science Symposium, Beijing.
Geospace Electrodynamic Connections (GEC) Mission The GEC mission has been in the formulation phase as part of NASA’s Solar Terrestrial Probe program for.
Probing the Ionosphere with Radioscience Instruments on CASSIOPE-e-POP Athabasca University - University of Alberta - University of Calgary - University.
1 FIREBIRD Science Overview Marcello Ruffolo Nathan Hyatt Jordan Maxwell 2 August 2013FIREBIRD Science.
Fine-scale 3-D Dynamics of Critical Plasma Regions: Necessity of Multipoint Measurements R. Lundin 1, I. Sandahl 1, M. Yamauchi 1, U. Brändström 1, and.
PHYSICS AND ENGINEERING PHYSICS Mohsen Ghezelbash, H. Liu, A.V. Koustov and D. André F-region echo occurrence in the polar cap: A comparison of PolarDARN.
Auroral dynamics EISCAT Svalbard Radar: field-aligned beam  complicated spatial structure (
Modeling Generation and Nonlinear Evolution of Plasma Turbulence for Radiation Belt Remediation Center for Space Science & Engineering Research Virginia.
Preliminary Results from the CASCADES 2 Sounding Rocket Paul Kintner, Eric Lundberg, Cornell U. Kristina Lynch, Meghan Mella, Dartmouth C. Nicolay Ivchencko,
HF Focusing due to Field Aligned Density Perturbations A. Vartanyan 1, G. M. Milikh 1, K. Papadopoulos 1, M. Parrot 2 1 Departments of Physics and Astronomy,
Alfvén Wave Generation and Dissipation Leading to High-Latitude Aurora W. Lotko Dartmouth College Genesis Fate Impact A. Streltsov, M. Wiltberger Dartmouth.
Boundaries in the auroral region --- Small scale density cavities and associated processes --- Vincent Génot (CESR/CNRS) C. Chaston (SSL) P. Louarn (CESR/CNRS)
Solar system science using X-Rays Magnetosheath dynamics Shock – shock interactions Auroral X-ray emissions Solar X-rays Comets Other planets Not discussed.
DOPPLER DOPPLER A Space Weather Doppler Imager Mission Concept Exploration Science Objectives What are the most relevant observational signatures of flare,
Global Distribution / Structure of Aurora Photograph by Jan Curtis Synthetic Aurora pre- midnight,multi-banded Resonant ULF waves produce pre- midnight,
CISM Advisory Council Meeting 4 March Ionosphere-Thermosphere Modeling Tim Killeen, Stan Solomon, and the CISM Ionosphere-Thermosphere Team.
Introduction Acknowledgement: Research at the University of New Hampshire was supported by NSF grants. E-POP Observations of Pulsating Aurora Bruce Fritz,
International Colloquium and Workshop "Ganymede Lander: scientific goals and experiments"
RESONANCE Project for Studies of Wave-Particle Interactions in the Inner Magnetosphere Anatoly Petrukovich and Resonance team RESONANCEРЕЗОНАНС R.
Measuring ITM Variability:Missions Around Geospace-Part 2 Jan J Sojka Center for Atmospheric and Space Sciences Utah State University, Logan, Utah
RUSSIAN SPACE MISSIONS FOR SOLAR-TERRESTRIAL SCIENCE ILWS-2011 A.A. Petrukovich, L.M. Zelenyi Space Research Institute V.D. Kuznetsov IZMIRAN.
China National Report , Prague, Czech Republic.
University of Colorado 1 ; Delft University of Technology 2 ; University of Alaska 3 ; Centre National d’Etudes Spatiales 4 ; National Center for Atmospheric.
Magnetosphere-Ionosphere coupling processes reflected in
An Auroral Imaging Mission for ILWS Eric Donovan - University of Calgary December 9, 2004 Acknowledgements: John Bonnell & Emma Spanswick Representing:
China National Report , Uppsala, Sweden China National Space Administration.
29 August, 2011 Beijing, China Space science missions related to ILWS in China
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.
Ionospheric Electrodynamics & Low-Earth Orbiting Satellites (LEOS) J-M Noël, A. Russell, D. Burrell & S. Thorsteinson Royal Military College of Canada.
In Situ Measurements of Auroral Acceleration Regions Wu Tong
Distributed Radar Networks Ray Greenwald JHU/APL.
Ionospheric Research at USU R.W. Schunk, L. Scherliess, J.J. Sojka, D.C. Thompson & L. Zhu Center for Atmospheric & Space Sciences Utah State University.
ESOC/CSSDP I/F Meeting October 25-26, 2007 Greg Enno – UofC.
Observing ion cyclotron waves M. R. Lessard, M. Widholm, P. Riley, H. Kim M. J. Engebretson University of New Hampshire Augsburg College NSF Workshop on.
Simulations of Radio Imaging in the Earth’s Magnetosphere J. L. Green, S. Boardsen, W. W. L. Taylor, S. F. Fung, R. F. Benson, B. Reinisch, and D. L. Gallagher.
ICS VIII Banff Canada March 27-31, 2006 To be convened by Eric Donovan & John Samson Shameless focus on THEMIS! To be held at the Banff Center Webpage.
1 MAVEN PFP ICDR May 23-25, 2011 Mars Atmosphere and Volatile EvolutioN (MAVEN) Mission Particles and Fields Science Critical Design Review May ,
Topics in Space Weather Earth Atmosphere & Ionosphere
Integrity  Service  Excellence Physics of the Geospace Response to Powerful HF Radio Waves HAARP-Resonance Workshop, 8-9 November 2011 Evgeny Mishin.
William Liu Canadian Space Agency June 12, 2007, Uppsala, Sweden CSA Report to the 5 th ILWS Working Group Meeting.
CRRES observations indicate an abrupt increase in radiation belt fluxes corresponding to the arrival of a solar wind shock. The processes(s) which accelerate.
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.
Numerical simulations of wave/particle interactions in inhomogeneous auroral plasmas Vincent Génot (IRAP/UPS/CNRS, Toulouse) F. Mottez (LUTH/CNRS, Meudon)
Mike Ruohoniemi 2012VT SuperDARN Remote Sensing of the Ionosphere and Earth’s Surface with HF Radar J. Michael Ruohoniemi and Joseph Baker.
Space Weather Canada: Addressing user needs LarisaTrichtchenko (NRCan) and Ian R. Mann (U. Alberta)
SS Special Section of JGR Space Physics Marks Polar’s 5th Anniversary September 4, 1996 This April special section is first of two Polar special sections.
Energy inputs from Magnetosphere to the Ionosphere/Thermosphere ASP research review Yue Deng April 12 nd, 2007.
Radiation Belt Storm Probes Mission and the Ionosphere-Thermosphere RPSP SWG Meeting June 2009.
near-Space Environment
Initial Results from the RENU2 Sounding Rocket
CAP congress, Ottawa, June 13-17, 2016
3rd Swarm Science Meeting, Copenhagen, 19 May 2014
Plasma Wave Excitation Regions in the Earth’s Global Magnetosphere
Connecting Earth to Space: NASA Heliophysics Provides Data on how Space Weather Impacts Earth’s Environment Using NASA Van Allen Probes mission data, researchers.
CEDAR Frontiers: Daytime Optical Aeronomy Duggirala Pallamraju and Supriya Chakrabarti Center for Space Physics, Boston University &
The Ionosphere and Thermosphere GEM 2013 Student Tutorial
Canadian Ground-Based Optical Programs
CEDAR Frontiers – Understanding the Polar Cap Ionosphere-Magnetosphere System Canadian High-Arctic Ionospheric Network (CHAIN) Jayachandran P. T., University.
Thermosphere-Ionosphere Issues for DASI - I:
RISR-C incoherent scatter radar operations
The ionosphere is much more structured and variable than ever predicted. Solar Driven Model Since 2000, we have seen more, very clear evidence that the.
Ionosphere, Magnetosphere and Thermosphere Anthea Coster
Solar and Heliospheric Physics
Earth’s Ionosphere Lecture 13
Satellite mission ideas using EISCAT_3D
Three Regions of Auroral Acceleration
Presentation transcript:

Andrew W. Yau University of Calgary, Canada CASSIOPE Enhanced Polar Outflow Probe (e-POP) University of Alberta, October 25, 2007

Outline 1.e-POP Mission Objective 2.CASSIOPE and e-POP 3.e-POP Science Targets 4.e-POP Mission Strategy 5.e-POP Instruments & Measurements 6.Conclusions

e-POP Mission Objective Observations of space weather processes –Micro- and meso-scale processes –In topside polar ionosphere –At highest possible resolution –Focus on plasma outflow, neutral escape, auroral currents, irregularities, radio propagation

The CASSIOPE Small Satellite e-POP Science Payload High resolution studies of space plasma processes; wave-particle interactions Small Satellite Bus Generic, low-cost bus for Canadian small-sat missions Cascade Tech Payload High bandwidth store-and- forward data delivery demo

ENHANCED POLAR OUTFLOW PROBE (e-POP) Science Plasma outflow Acceleration; WPI; auroral connection Wave propagation 3D structure of ionospheric irregularities Neutral escape Temperature enhancement, non-thermal escape Mission Concept Highest-resolution in-situ measurements Radio wave propagation 3D studies Fast imaging of meso-scale aurora Mission Design Polar orbit: 325 × 1500 km; 80° incl. 3-axis stabilized Large data storage and downlink bandwidth (>1 TB, 300 Mbps)

Science Objective #1: Plasma Outflow Facts Significant energetic ionospheric ion injection to magnetosphere: ≥10 26 s -1 Topside polar ionosphere is source of multiple “cold” ion populations Questions Cold ions and driving processes: What is (are) the critical first step(s) in ionosphere- magnetosphere mass transfer? e-POP Objectives Plasma outflow and waves: Micro-scale ion upflow/acceleration; wave particle interaction; auroral connection

Science Objective #2: Radio Propagation Facts Plasma can refract, scatter, amplify, damp, or decompose electromagnetic waves. Refraction depends on ionospheric conditions. Questions How does M-I energy-mass coupling manifest in ionospheric irregularities? How do irregularities interact with waves - and affect radio wave propagation? SuperDARN e-POP Objectives Waves propagation in plasma: 3D structure of ionospheric irregularities; radio/GPS occultation studies

Science Objective #3: Neutral Escape Facts Charged/neutral H, He, and O rapidly charge- exchange in laboratory – and in space Questions Role of thermosphere in magnetosphere- ionosphere-thermosphere mass transfer? e-POP Objectives Explore neutral atmospheric escape: Temperature enhancement; non-thermal escape

ENHANCED POLAR OUTFLOW PROBE (e-POP) Science Plasma outflow Acceleration; WPI; auroral connection Wave propagation 3D structure of ionospheric irregularities Neutral escape Temperature enhancement, non-thermal escape Mission Concept Highest-resolution in-situ measurements Radio wave propagation 3D studies Fast imaging of meso-scale aurora Mission Design Polar orbit: 325 × 1500 km; 80° incl. 3-axis stabilized Large data storage and downlink bandwidth (>1 TB, 300 Mbps)

Sub-Decameter Scale Structures in Topside Ionosphere MARIE rocket, km altitude, large substorm (LaBelle 1986) “Spikelets” –Localized lower hybrid waves –Lower hybrid solitary structures Often coincided with localized regions of TAI (“perpendicular ion conics”)  1 ms time scale and/or  1 m horizontal/vertical extent

Dynamic Small-scale Structures in Visual Aurora Auroral spatial scales: km (bands), to km (curtains) Auroral curls (Trondsen 1998): –1-2 km spatial scale –Anti-clockwise rotation and motion (when viewed anti-parallel to B)  13.5 km   10.1 km   10.8 km  W N

ENHANCED POLAR OUTFLOW PROBE (e-POP) Science Plasma outflow Acceleration; WPI; auroral connection Wave propagation 3D structure of ionospheric irregularities Neutral escape Temperature enhancement, non-thermal escape Mission Concept Highest-resolution in-situ measurements Radio wave propagation 3D studies Fast imaging of meso-scale aurora Mission Design Polar orbit: 325 × 1500 km; 80° incl. 3-axis stabilized Large data storage and downlink bandwidth (>1 TB, 300 Mbps)

FAI e-POP Instrument Complement Name InstrumentPIMeasurements IRM Imaging and rapid ion mass spectrometer Calgary Amerl eV ions SEI Suprathermal electron imager Calgary Knudsen eV electrons NMS Neutral mass and velocity spectrometer JAXA/ISAS Hayakawa km/s neutrals MGF Magnetic field instrumentCalgary Wallis  B  j // RRI Radio receiver instrumentCRC James HF, VLF E(  ), k(  ) GAP GPS attitude, position, and profiling experiment UNB Langley L1, L2  Irregularity CER Coherent electromagnetic radio tomography NRL Bernhardt VHF  Irregularity FAI Fast auroral imagerCalgary Murphree 630 nm, NIR IRM SEI CER NMS RRI MGF GAP In-situ Instruments

e-POP Instrument Complement Name InstrumentPIMeasurements IRM Imaging and rapid ion mass spectrometer Calgary Amerl eV ions SEI Suprathermal electron imager Calgary Knudsen eV electrons NMS Neutral mass and velocity spectrometer JAXA/ISAS Hayakawa km/s neutrals MGF Magnetic field instrumentCalgary Wallis  B  j // RRI Radio receiver instrumentCRC James E, k: HF, VLF (10 Hz –18 MHz) GAP GPS attitude, position, and profiling experiment UNB Langley L1, L2  Irregularity CER Coherent electromagnetic radio tomography NRL Bernhardt VHF  Irregularity FAI Fast auroral imagerCalgary Murphree 630 nm, NIR IRM SEI CER FAI NMS RRI MGF GAP Radio Instruments

e-POP Instrument Complement Name InstrumentPIMeasurements IRM Imaging and rapid ion mass spectrometer Calgary Amerl eV ions SEI Suprathermal electron imager Calgary Knudsen eV electrons NMS Neutral mass and velocity spectrometer JAXA/ISAS Hayakawa km/s neutrals MGF Magnetic field instrumentCalgary Wallis  B  j // RRI Radio receiver instrumentCRC James HF, VLF E(  ), k(  ) GAP GPS attitude, position, and profiling experiment UNB Langley L1, L2  Irregularity CER Coherent electromagnetic radio tomography NRL Bernhardt VHF  Irregularity FAI Fast auroral imagerCalgary Murphree 630 nm, NIR IRM SEI CER FAI NMS RRI MGF GAP Auroral Imager

e-POP Science Team and Partner Organizations Communications Research Centre: HG James, P Prikryl Royal Military College: JM Noel U. Alberta: R Rankin, C Watt U. Athabasca: M Connors U. Calgary: PV Amerl, LL Cogger, E Donovan, DJ Knudsen, JS Murphree, TT Trondsen, DD Wallis, AW Yau U. New Brunswick: A Hamza, PT Jayachandran, D Kim, R Langley U. Saskatchewan: G Hussey, S Koustov, G Sofko, JP St Maurice U. Victoria: RE Horita U. Western Ontario: L Kagan, J MacDougall York U: JG Laframboise, J McMahon JAXA/ISAS, Japan: T Abe, H Hayakawa, K Tsuruda NRL, USA: PA Bernhardt, C Siefring UNH, USA: M Lessard

Conclusions e-POP … Part of multi-purpose CASSIOPE mission Mission objective: highest-resolution space weather observation –Plasma outflow, wave propagation, and neutral escape Payload: 8 plasma, field, optical, radio instruments Focus: hi-res particle/wave observations and fast auroral imaging Use non-spinning orbiter, large data storage, fast downlink Coordinated operation with ground facilities an essential element

For more information, please visit: Thank You!

Lower Hybrid Solitary Structures in Topside Ionosphere LHSS signatures –Density depletion –TAI and/or BB VLF noise GEODESIC rocket, 980 km (Burchill 2004) Low-energy ion distributions –11 ms/13 m resolution –T  0.2 eV (rammed O + ions) –Heated ions at several eV Observed density cavity –  15% depletion –Temporal extent:  10 ms

LHSS “Heating” Width “Heating” width of LHSS on GEODESIC –from velocity images Average width: 63 m Standard dev.: 25 m Range: 13 – 190 m “Density depletion” width  20 m Burchill et al., 2004