URSIGA, New Delhi, 23-29 Oct 2005 Coordinated Observations of Ionospheric Scintillations, Density Profiles and Total Electron Content on a Common Magnetic.

Slides:



Advertisements
Similar presentations
Modelling complexity in the upper atmosphere using GPS data Chris Budd, Cathryn Mitchell, Paul Spencer Bath Institute for Complex Systems, University of.
Advertisements

University of Bath 4D ionisation dynamics during storms of the recent solar maximum Cathryn Mitchell, Ping Yin, Paul Spencer and Dmitriy Pokhotelov, University.
ESWW 5 Some ionospheric effects on ground based radar Y. Béniguel, J.-P. Adam.
B-spline Model of Ionospheric Scintillation
HF management communication system and link optimization Bruno Zolesi. Istituto Nazionale di Geofisica e Vulcanologia.
M. Gende 1,2, C. Brunini 1,2, F. Azpilicueta 1,2 Universidad Nacional de La Plata, Argentina 1 CONICET, Argentina 2 La Plata Ionospheric Model as a tool.
The day-to-day longitudinal variability of the global ionospheric density distribution: Preliminary results E.E. Pacheco and E. Yizengaw Institute for.
Preeti Bhaneja Terry Bullett November 8, 2011
Using a DPS as a Coherent Scatter HF Radar Lindsay Magnus Lee-Anne McKinnell Hermanus Magnetic Observatory Hermanus, South Africa.
The Challenges of Validating Global Assimilative Models of the Ionosphere L.F. M c Namara 1,C.R. Baker 2, G.J. Bishop 2, D.T. Decker 2, J.A. Welsh 2 1.
Comparative Study of the Global Ionospheric Behavior During Solar Cycles and Minima Eduardo A. Araujo-Pradere 1,2, Dominic Fuller-Rowell 1,3,
The Surface-based Temperature Inversion on the Antarctic Plateau Stephen R. Hudson and Richard E. Brandt University of Washington Contact Information:
Observation of Equatorial Electrodynamics in Africa using AMBER Magnetometer Network Endawoke Yizengaw Institute for Scientific Research, Boston College,
Storm-time total electron content and its response to penetration electric fields over South America P. M. de Siqueira, E. R. de Paula, M. T. A. H. Muella,
The North East CIDR Array (NECA): A Chain of Ionospheric Tomography Receivers for Studying the Equatorward Edge of the Auroral Oval and the Mid-latitude.
Space Weather Workshop, Boulder, CO, April 2013 No. 1 Ionospheric plasma irregularities at high latitudes as observed by CHAMP Hermann Lühr and.
Titan’s Thermospheric Response to Various Plasma Environments Joseph H. Westlake Doctoral Candidate The University of Texas at San Antonio Southwest Research.
Abstract Since the ionosphere is the interface between the Earth and space environments and impacts radio, television and satellite communication, it is.
SCHOOL OF PHYSICS Space Weather in the Equatorial Ionosphere Robert Stening School of Physics, University of New South Wales Acknowledge help from Dr J.
Global Distribution / Structure of Aurora Photograph by Jan Curtis Synthetic Aurora pre- midnight,multi-banded Resonant ULF waves produce pre- midnight,
Mesoscale ionospheric tomography over Finland Juha-Pekka Luntama Finnish Meteorological Institute Cathryn Mitchell, Paul Spencer University of Bath 4th.
TIMED-GUVI for Nowcasting R. A. Goldberg and J. B. Sigwarth
1 UNCLASSIFIED – FOUO – Not for Public Release Operational Space Environment Network Display (OpSEND) & the Scintillation Network Decision Aid Dr. Keith.
Antarctic Peninsula is a very suitable area for experimental investigations of troposphere-to-ionosphere energy transfer because this place characterized.
Sandro M. Radicella Head, Aeronomy and radiopropagation Laboratory Ionospheric Research at the Abdus Salam ICTP Aeronomy and Radiopropagation Laboratory.
Nighttime 4-peak Longitudinal Structure of Ionospheric Plasma Density at Mid-Low latitudes During High and Extreme.
ARL Applied Research Laboratories The University of Texas at Austin ARL Applied Research Laboratories The University of Texas at Austin Ionospheric Tomography.
1 Using Hemispheric-CMAQ to Provide Initial and Boundary Conditions for Regional Modeling Joshua S. Fu 1, Xinyi Dong 1, Kan Huang 1, and Carey Jang 2 1.
Modern Era Retrospective-analysis for Research and Applications: Introduction to NASA’s Modern Era Retrospective-analysis for Research and Applications:
The climate and climate variability of the wind power resource in the Great Lakes region of the United States Sharon Zhong 1 *, Xiuping Li 1, Xindi Bian.
Distributed Radar Networks Ray Greenwald JHU/APL.
Charles S. Carrano, Cesar E. Valladares, Keith M. Groves
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.
VARIABILITY OF TOTAL ELECTRON CONTENT AT EUROPEAN LATITUDES A. Krankowski(1), L. W. Baran(1), W. Kosek (2), I. I. Shagimuratov(3), M. Kalarus (2) (1) Institute.
The Mesoscale Ionospheric Simulation Testbed (MIST) Regional Data Assimilation Model Joseph Comberiate Michael Kelly Ethan Miller June 24, 2013.
Comparison of the electron density profiles measured with the Incoherent Scatter Radar, Digisonde DPS-4 and Chirp-Ionosonde Ratovsky K.G., Shpynev* B.G.,
The Thermosphere/Ionosphere Response to Solar Activity During the October/November 2003 Storms P. R. Straus 1, G. Crowley 2, R. R. Meier 3, L. J. Paxton.
Guan Le NASA Goddard Space Flight Center Challenges in Measuring External Current Systems Driven by Solar Wind-Magnetosphere Interaction.
Diurnal Water and Energy Cycles over the Continental United States from three Reanalyses Alex Ruane John Roads Scripps Institution of Oceanography / UCSD.
Ionospheric irregularities observed with a GPS network in Japan TOHRU ARAMAKI[1],Yuichi Otsuka[1],Tadahiko Ogawa[1],Akinori Saito[2] and Takuya Tsugawa[2]
Global Structure of the Inner Solar Wind and it's Dynamic in the Solar Activity Cycle from IPS Observations with Multi-Beam Radio Telescope BSA LPI Chashei.
Predicting Ionospheric Densities and Scintillation with the Communication / Navigation Outage Forecasting System (C/NOFS) Mission Chin S. Lin 1, O. de.
Electron density profile retrieval from RO data Xin’an Yue, Bill Schreiner  Abel inversion error of Ne  Data Assimilation test.
Data Assimilation Retrieval of Electron Density Profiles from Radio Occultation Measurements Xin’an Yue, W. S. Schreiner, Jason Lin, C. Rocken, Y-H. Kuo.
0 7th ESWW, Bruges, Ionospheric Scintillations Propagation Model Y. Béniguel, J-P Adam IEEA, Courbevoie, France.
COSMIC Ionospheric measurements Jiuhou Lei NCAR ASP/HAO Research review, Boulder, March 8, 2007.
© Copyright QinetiQ limited 2006 On the application of meteorological data assimilation techniques to radio occultation measurements of.
Real time reconstruction of 3-D electron density distribution over Europe with TaD profiler Ivan Kutiev 1,2, Pencho Marinov 1, Anna Belehaki 2 1 Bulgarian.
1 AIR FORCE RESEARCH LABORATORY Dr. Keith Groves Space Weather Center of Excellence AFRL/VSBXI 29 Randolph Rd Hanscom AFB, MA voice
Characteristics and source of the electron density irregularities in the Earth’s ionosphere Hyosub Kil Johns Hopkins University / Applied Physics Laboratory.
Effects of January 2010 stratospheric sudden warming in the low-latitude ionosphere L. Goncharenko, A. Coster, W. Rideout, MIT Haystack Observatory, USA.
30 April 2009 Space Weather Workshop 2009 The Challenge of Predicting the Ionosphere: Recent results from CISM. W. Jeffrey Hughes Center for Integrated.
NATIONAL INSTITUTE FOR SPACE RESEARCH – INPE/MCT SOUTHERN REGIONAL SPACE RESEARCH CENTER – CRS/CCR/INPE – MCT FEDERAL UNIVERSITY OF SANTA MARIA - UFSM.
Solar Radio Bursts and Effects on GPS*
Global and Regional Total Electron Content Anthony Mannucci, Xing Meng, Panagiotis Vergados, Attila Komjathy JPL/Caltech Collaborators: Sarah E. McDonald,
JMA Report on Satellite-based Space Weather Activities in Japan
The 3rd Swarm Science Meeting, June 2014, Copenhagen, Denmark
Bruce Cornuelle, Josh Willis, Dean Roemmich
S. Datta-Barua, Illinois Institute of Technology G. S. Bust, JHUAPL
Status of GNSS ionospheric Study in Korea
Atmosphere-Ionosphere Wave Coupling as Revealed in Swarm Plasma Densities and Drifts Jeffrey M. Forbes Department of Aerospace Engineering Sciences, University.
Overview of Downscaling
First validation of Level 2 CAT-2 products: FAC/IBI/TEC
Center for Atmospheric & Space Sciences
Ionosphere, Magnetosphere and Thermosphere Anthea Coster
Aura Science Team meeting
An overview of the ionospheric research at INPE, Brazil
GPS Ionospheric Mapping at Natural Resources Canada
Evaluation of IRI-2012 by comparison with JASON-1 TEC and incoherent scatter radar observations during the solar minimum period Eun-Young Ji,
NASA’s Global-scale Observations of the Limb and Disk (GOLD) Mission: Unprecedented Imaging of the Boundary Between Earth and Space Richard Eastes GOLD.
Presentation transcript:

URSIGA, New Delhi, Oct 2005 Coordinated Observations of Ionospheric Scintillations, Density Profiles and Total Electron Content on a Common Magnetic Flux Tube K. M. Groves 1, S. Basu 1, T. R. Pedersen 1 T. L. Beach 1, J. M. Quinn 1, B. Taliaferro 1 E. R. de Paula, I. S. Batista, M. A. Abdu, R.C. Livingston, P. Ning, C. Carrano 1 Space Vehicles Directorate Space Weather Center of Excellence Air Force Research Laboratory 2005 URSI General Assembly, New Delhi, India GF1B: Atmosphere-Ionosphere Sounding by Using Global Navigation Satellite Systems

URSIGA, New Delhi, Oct 2005 Spread F Meridional Dependence Motivation: Regional specification from 1-D measurements COPEX Campaign Overview Ionospheric variations at conjugate locations Summary Outline

URSIGA, New Delhi, Oct 2005 Data Assimilation Methods Constraining model output Developing statistical interpolation techniques Adjusting model drivers –Kalman filter –Adjoint methods Real-time Scintillation Nowcasting from Space The satellite provides only a one-dimensional sampling of the parameters. Need to specify the ionosphere in 3-D Communication/Navigation Outage Forecast System (C/NOFS)

URSIGA, New Delhi, Oct 2005 Motivation: Observation Extrapolation The Challenge: Map 1-D scintillation estimates into 2-D representations Satellite measurement ground track Current assumption: Symmetry about the magnetic equator— Inconsistent with asymmetric density structure near solstice Simulated scintillation structures

URSIGA, New Delhi, Oct 2005 COPEX Campaign Oct-Nov 2002 Magnetic equator & conjugate location observations Conducted by INPE with AFRL & University collaboration Objective is to understand initiation, growth and dynamics of young plume structures Critical to understanding large- scale structure of depletion development Multi-diagnostics at three locations will measure required ionospheric parameters

URSIGA, New Delhi, Oct 2005 Principal Instrumentation Instruments operated from Oct to 07 Dec 2002 Sites on common flux tube; Campo Grande and Boa Vista magnetically conjugate Combination of these data with available ROCSAT passes and other ancillary data sets provide basis to investigate meridional variations in detail Campo GrandeCachimbo/ *Alta FlorestaBoa Vista Digisonde VHF scint & drift GPS TEC & scint All-sky imager Digisonde VHF scint & drift GPS TEC & scint All-sky imager Digisonde VHF scint & drift* GPS TEC & scint* All-sky imager VHF coherent backscatter radar* GEO 20.5S 54.7W 9.5S 54.8W/ 9.9S 56.1W 2.8N 60.7W MAG 10.8S 14.0E 0.7S 15.2E 12.6N 13.5E

URSIGA, New Delhi, Oct 2005 Mlat VTEC TEC Structure Oct-Nov 2002 TEC data reveals asymmetric anomaly structure driven by inter- hemispheric neutral wind Mean TEC levels decreasing ~30%+ from October to December Local Time VTEC Mlat Local Time VTEC October 3-9 November 1-7 December

URSIGA, New Delhi, Oct 2005 Mlat S4 S4 Structure Oct-Nov 2002 GPS L1 (1575 MHz) Scintillation Scintillation activity and intensity peak in December despite ~20% decrease in overall peak density Scintillation intensity symmetric as a function of magnetic latitude Local Time S4 Mlat Local Time S October 3-9 November 1-7 December

URSIGA, New Delhi, Oct 2005 Examine daily plots between UT (~ LT) No observations below 30° elevation angle used in analysis Consider results statistically when scintillation occurred and data was present at both “high latitude” stations CGR AFL BVB Analysis Approach

URSIGA, New Delhi, Oct 2005 TEC Characterization Overall TEC decreases 20-50% from October to December Largest decreases observed in southern anomaly North/South TEC ratio increases from 1.2 in October to about 1.4 in December (40% higher!) Avg TEC UT North/South Ratio

URSIGA, New Delhi, Oct 2005 Peak Density Characterization On average, F0F2 remains relatively constant over observing period Largest decreases observed in southern anomaly North/South F0F2 ratio increases from unity in October to about 1.1 in December (approximately 20% higher peak density) Variations increase significantly during latter half of campaign –May be related to reading ionograms with increased spread F Avg F0F UT North/South F0F2 Ratio

URSIGA, New Delhi, Oct 2005 Slab Thickness Effective slab thickness (TEC/NmF2) exhibits similar decrease over time Thicknesses generally 10-20% greater in northern hemisphere, becoming quite variable during 2 nd half of campaign (Nov-Dec) Avg Slab Thickness UT North/South Slab Thickness Ratio

URSIGA, New Delhi, Oct 2005 What About Scintillation? ~10% decrease in S4 (   N) over campaign period not entirely consistent with decrease in NmF2 (~20%) North/south ratio is essentially unity (no asymmetry)

URSIGA, New Delhi, Oct 2005 Statistical View Distribution of scintillation activity and intensity are statistically identical in both hemispheres despite differences in TEC and, to lesser extent, F0F2 Activity increases in frequency during latter half of campaign Intensity distribution is essentially unchanged (2-3% decrease in monthly statistics) 795 Samples Percentile S4 25: : : : Samples Percentile S4 25: : : : Samples Percentile S4 25: : : : Samples Percentile S4 25: : : : a)b) c) d)

URSIGA, New Delhi, Oct 2005 Scintillation intensity appears relatively independent of background TEC variations near the anomaly crests TEC decreases markedly approaching summer solstice, particularly in the southern magnetic hemisphere; change in NmF2 less than half observed TEC decrease On average TEC, NmF2 and slab thickness greater in the northern magnetic hemisphere during this time period (Oct- Dec 2002) S4 appears to be essentially symmetric at the same magnetic latitude in both hemispheres, despite variations in TEC, slab thickness, and NmF2 Vertical distribution of irregularities non-homogenous; propagation effects dominated by layer near F-region peak Conclusions