Solar Radar Experiments

Similar documents
Modeling of Ionospheric Refraction of UHF Radar Signals at High Latitudes

Investigation of a Forward Looking Conformal Broadband Antenna for Airborne Wide Area Surveillance

INTEGRATIVE MIGRATORY BIRD MANAGEMENT ON MILITARY BASES: THE ROLE OF RADAR ORNITHOLOGY

A RENEWED SPIRIT OF DISCOVERY

A Comparison of Two Computational Technologies for Digital Pulse Compression

Coherent distributed radar for highresolution

Ship echo discrimination in HF radar sea-clutter

RF Performance Predictions for Real Time Shipboard Applications

Assimilation Ionosphere Model

The Energy Spectrum of Accelerated Electrons from Waveplasma Interactions in the Ionosphere

Key Issues in Modulating Retroreflector Technology

COM DEV AIS Initiative. TEXAS II Meeting September 03, 2008 Ian D Souza

Remote Sediment Property From Chirp Data Collected During ASIAEX

Non-Data Aided Doppler Shift Estimation for Underwater Acoustic Communication

Modeling Antennas on Automobiles in the VHF and UHF Frequency Bands, Comparisons of Predictions and Measurements

Strategic Technical Baselines for UK Nuclear Clean-up Programmes. Presented by Brian Ensor Strategy and Engineering Manager NDA

Sky Satellites: The Marine Corps Solution to its Over-The-Horizon Communication Problem

Underwater Intelligent Sensor Protection System

Innovative 3D Visualization of Electro-optic Data for MCM

SA Joint USN/USMC Spectrum Conference. Gerry Fitzgerald. Organization: G036 Project: 0710V250-A1

PULSED BREAKDOWN CHARACTERISTICS OF HELIUM IN PARTIAL VACUUM IN KHZ RANGE

Durable Aircraft. February 7, 2011

IDA3D: An Ionospheric Data Assimilative Three Dimensional Tomography Processor

THE CREATION OF DIFFERENTIAL CORRECTION SYSTEMS AND THE SYSTEMS OF GLOBAL NAVIGATION SATELLITE SYSTEM MONITORING

Radar Detection of Marine Mammals

Presentation to TEXAS II

Acoustic Monitoring of Flow Through the Strait of Gibraltar: Data Analysis and Interpretation

LONG TERM GOALS OBJECTIVES

Satellite Observations of Nonlinear Internal Waves and Surface Signatures in the South China Sea

Marine Mammal Acoustic Tracking from Adapting HARP Technologies

Signal Processing Architectures for Ultra-Wideband Wide-Angle Synthetic Aperture Radar Applications

Range-Depth Tracking of Sounds from a Single-Point Deployment by Exploiting the Deep-Water Sound Speed Minimum

GLOBAL POSITIONING SYSTEM SHIPBORNE REFERENCE SYSTEM

PULSED POWER SWITCHING OF 4H-SIC VERTICAL D-MOSFET AND DEVICE CHARACTERIZATION

Report Documentation Page

VHF/UHF Imagery of Targets, Decoys, and Trees

North Pacific Acoustic Laboratory (NPAL) Towed Array Measurements

NPAL Acoustic Noise Field Coherence and Broadband Full Field Processing

Technology Maturation Planning for the Autonomous Approach and Landing Capability (AALC) Program

Two-Way Time Transfer Modem

August 9, Attached please find the progress report for ONR Contract N C-0230 for the period of January 20, 2015 to April 19, 2015.

Using Radio Occultation Data for Ionospheric Studies

IREAP. MURI 2001 Review. John Rodgers, T. M. Firestone,V. L. Granatstein, M. Walter

TRANSMISSION LINE AND ELECTROMAGNETIC MODELS OF THE MYKONOS-2 ACCELERATOR*

Ground Based GPS Phase Measurements for Atmospheric Sounding

Bistatic Underwater Optical Imaging Using AUVs

Evanescent Acoustic Wave Scattering by Targets and Diffraction by Ripples

DIELECTRIC ROTMAN LENS ALTERNATIVES FOR BROADBAND MULTIPLE BEAM ANTENNAS IN MULTI-FUNCTION RF APPLICATIONS. O. Kilic U.S. Army Research Laboratory

ULTRASTABLE OSCILLATORS FOR SPACE APPLICATIONS

Acoustic Measurements of Tiny Optically Active Bubbles in the Upper Ocean

Ocean Acoustics and Signal Processing for Robust Detection and Estimation

A New Scheme for Acoustical Tomography of the Ocean

Adaptive CFAR Performance Prediction in an Uncertain Environment

RADAR SATELLITES AND MARITIME DOMAIN AWARENESS

CFDTD Solution For Large Waveguide Slot Arrays

Loop-Dipole Antenna Modeling using the FEKO code

U.S. Army Training and Doctrine Command (TRADOC) Virtual World Project

Measurement of Ocean Spatial Coherence by Spaceborne Synthetic Aperture Radar

Lattice Spacing Effect on Scan Loss for Bat-Wing Phased Array Antennas

Report Documentation Page

Best Practices for Technology Transition. Technology Maturity Conference September 12, 2007

SYSTEMATIC EFFECTS IN GPS AND WAAS TIME TRANSFERS

Investigation of Modulated Laser Techniques for Improved Underwater Imaging

Oceanographic and Bathymetric Effects on Ocean Acoustics

Modeling an HF NVIS Towel-Bar Antenna on a Coast Guard Patrol Boat A Comparison of WIPL-D and the Numerical Electromagnetics Code (NEC)

HF Radar Measurements of Ocean Surface Currents and Winds

Department of Defense Partners in Flight

Oceanographic Variability and the Performance of Passive and Active Sonars in the Philippine Sea

Hybrid QR Factorization Algorithm for High Performance Computing Architectures. Peter Vouras Naval Research Laboratory Radar Division

RECENT TIMING ACTIVITIES AT THE U.S. NAVAL RESEARCH LABORATORY

Marine~4 Pbscl~ PHYS(O laboratory -Ip ISUt

Argus Development and Support

Frequency Stabilization Using Matched Fabry-Perots as References

14. Model Based Systems Engineering: Issues of application to Soft Systems

INFRASOUND SENSOR MODELS AND EVALUATION. Richard P. Kromer and Timothy S. McDonald Sandia National Laboratories

PHASING CAPABILITY. Abstract ARRAY. level. up to. to 12 GW. device s outpu antenna array. Electric Mode. same physical dimensions.

REPORT DOCUMENTATION PAGE. Thermal transport and measurement of specific heat in artificially sculpted nanostructures. Dr. Mandar Madhokar Deshmukh

3D Propagation and Geoacoustic Inversion Studies in the Mid-Atlantic Bight

Department of Energy Technology Readiness Assessments Process Guide and Training Plan

ESME Workbench Enhancements

EFFECTS OF ELECTROMAGNETIC PULSES ON A MULTILAYERED SYSTEM

Passive Localization of Multiple Sources Using Widely-Spaced Arrays With Application to Marine Mammals

Modeling and Evaluation of Bi-Static Tracking In Very Shallow Water

Effects of Radar Absorbing Material (RAM) on the Radiated Power of Monopoles with Finite Ground Plane

Acoustic Horizontal Coherence and Beamwidth Variability Observed in ASIAEX (SCS)

Characteristics of an Optical Delay Line for Radar Testing

DESIGNOFASATELLITEDATA MANIPULATIONTOOLIN ANDFREQUENCYTRANSFERSYSTEM USING SATELLITES

Rump Session: Advanced Silicon Technology Foundry Access Options for DoD Research. Prof. Ken Shepard. Columbia University

Design of Synchronization Sequences in a MIMO Demonstration System 1

David Siegel Masters Student University of Cincinnati. IAB 17, May 5 7, 2009 Ford & UM

Effects of Fiberglass Poles on Radiation Patterns of Log-Periodic Antennas

SILICON CARBIDE FOR NEXT GENERATION VEHICULAR POWER CONVERTERS. John Kajs SAIC August UNCLASSIFIED: Dist A. Approved for public release

NEURAL NETWORKS IN ANTENNA ENGINEERING BEYOND BLACK-BOX MODELING

Reduced Power Laser Designation Systems

COMMON-VIEW TIME TRANSFER WITH COMMERCIAL GPS RECEIVERS AND NIST/NBS-TYPE REXEIVERS*

JOCOTAS. Strategic Alliances: Government & Industry. Amy Soo Lagoon. JOCOTAS Chairman, Shelter Technology. Laura Biszko. Engineer

REPORT DOCUMENTATION PAGE. A peer-to-peer non-line-of-sight localization system scheme in GPS-denied scenarios. Dr.

Diver-Operated Instruments for In-Situ Measurement of Optical Properties

0.18 μm CMOS Fully Differential CTIA for a 32x16 ROIC for 3D Ladar Imaging Systems

Development of a charged-particle accumulator using an RF confinement method FA

Transcription:

Solar Radar Experiments Paul Rodriguez Plasma Physics Division Naval Research Laboratory Washington, DC 20375 phone: (202) 767-3329 fax: (202) 767-3553 e-mail: paul.rodriguez@nrl.navy.mil Award # N0001498WX30228 LONG-TERM GOAL My long term goal is to develop the techniques to be used to reliably detect coronal mass ejections (CMEs) from the sun which are directed at the earth. The radar detection technique could provide several days advance notice of possible strong geomagnetic storms at earth. OBJECTIVES I wish to establish whether the Doppler shift of the radar echo can be measured and from that the earthward-directed velocity determined. The frequency of the radar signal that is launched from earth is such that CMEs would be detected in the range of 1 to 5 solar radii. The CME is detected while still in the solar corona and, based on the typical velocities of CMEs, will take several days to reach the earth s orbit. Such advance warning time makes it possible for space-based and ground-based systems that are vulnerable to geomagnetic storms to take some protective action. APPROACH Experiments have been conducted using Russian and Ukrainian research facilities that are close equivalents to an operational solar radar. The Russian facility is the SURA ionospheric heater, which is used as the radar transmitter at about 9 MHz and with total power of about 750 kw. The Ukrainian UTR-2 radio astronomy receiving array is used as the receiver of solar coronal echoes. The facilities are separated by about 1000 km; thus, they are used in bistatic mode. In order to investigate the effect of the earth s ionosphere on the transmitted and echo signal, we have also conducted experiments of direct transmission to the NASA WIND satellite and reflection from the moon. WORK COMPLETED Three summer campaigns, each of about two weeks duration in which about ten daily experiment have been conducted. The experiments are constrained by the elevation of sun in the sky, which must be above about 50 in the sky in order for the sun to be in the beam of the SURA transmitter. These requirement limit experiments to several weeks in summer. The dates of the campaigns are: 9-12 July 1996 19 July 25 August, 1997 10 June 25 July, 1998.

Report Documentation Page Form Approved OMB No. 0704-0188 Public reporting burden for the collection of information is estimated to average 1 hour per response, including the time for reviewing instructions, searching existing data sources, gathering and maintaining the data needed, and completing and reviewing the collection of information. Send comments regarding this burden estimate or any other aspect of this collection of information, including suggestions for reducing this burden, to Washington Headquarters Services, Directorate for Information Operations and Reports, 1215 Jefferson Davis Highway, Suite 1204, Arlington VA 22202-4302. Respondents should be aware that notwithstanding any other provision of law, no person shall be subject to a penalty for failing to comply with a collection of information if it does not display a currently valid OMB control number. 1. REPORT DATE 1998 4. TITLE AND SUBTITLE Solar Radar Experiments 2. REPORT TYPE 3. DATES COVERED 00-00-1998 to 00-00-1998 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6. AUTHOR(S) 5d. PROJECT NUMBER 5e. TASK NUMBER 5f. WORK UNIT NUMBER 7. PERFORMING ORGANIZATION NAME(S) AND ADDRESS(ES) Naval Research Laboratory,Plasma Physics Division,Washington,DC,20375 8. PERFORMING ORGANIZATION REPORT NUMBER 9. SPONSORING/MONITORING AGENCY NAME(S) AND ADDRESS(ES) 10. SPONSOR/MONITOR S ACRONYM(S) 12. DISTRIBUTION/AVAILABILITY STATEMENT Approved for public release; distribution unlimited 13. SUPPLEMENTARY NOTES See also ADM002252. 14. ABSTRACT 11. SPONSOR/MONITOR S REPORT NUMBER(S) 15. SUBJECT TERMS 16. SECURITY CLASSIFICATION OF: 17. LIMITATION OF ABSTRACT a. REPORT b. ABSTRACT c. THIS PAGE Same as Report (SAR) 18. NUMBER OF PAGES 4 19a. NAME OF RESPONSIBLE PERSON Standard Form 298 (Rev. 8-98) Prescribed by ANSI Std Z39-18

Because the solar echo signal is necessarily weak, data analysis has had to contend with relatively low signal-to-noise ratios (typically ~ 1 db). The analyses must therefore rely on integration techniques. In addition, we have tested various transmission coding approaches to help discriminate against background noise. The frequency of transmission (~9 MHz) is on the lower limit of the range of frequencies that should be used with solar radars; however, at present the SURA facility cannot transmit at higher frequency. RESULTS Thus far we have determined that in two cases, we have detected an echo signal from the solar corona. These cases have been when the background interference was relatively low. In the figure below, we show the data from the experiment of 21 July 1996. The pattern of ON-OFF pulses at two frequencies transmitted for 16 minutes is shown in the upper part of the figure. The integrated spectrum of solar corona echo as detected in ~40 khz bandwidth in the following 16 minutes is shown in the bottom part of the figure. The integrated spectrum power has approximately the same phase relationship as the transmitted pulses, thus identifying the echo signal.

IMPACT/APPLICATION The means by which we have conducted these solar radar experiments is appropriate for the design and construction of a future solar radar facility in the United States. The information gained and experience acquired are important for determining the requirements of such a solar radar. The United States presently has no solar radar, although the technology is readily available. TRANSITIONS A US solar radar would provide an important component for Space Weather forecasting of solarinduced geomagnetic storms, thus providing significant advance (several days) warning to operators of space and ground systems such as communications satellites and electric power grids. RELATED PROJECTS Studies with the HAARP radar facility being constructed in Alaska are conducted with the WIND spacecraft to study the effects of HF propagation over long distances in the earth s magnetosphere. These experiments provide new information on wave-plasma interactions and also are assessing the possible use of HAARP as a solar radar. REFERENCES James, J. C., Radar studies of the sun, in Radar Astronomy, ed. J. V. Evans and T. Hagfors, McGraw- Hill Book Company, New York, 1968. PUBLICATIONS Rodriguez, P., High frequency radar detection of coronal mass ejections, in Solar Drivers of Interplanetary and Terrestrial Disturbances, Astron. Soc. Pacific Conf. Series, Vol. 95, ed. K. S. Balasubramaniam, S. L. Kiel, and R. N. Smartt, pp. 180-188, 1996.