ANISOTROPY IN OCEAN SCATTERING OF BISTATIC RADAR USING SIGNALS OF OPPORTUNITY Rashmi Shah*, Dr. James Garrison*, Dr. Michael Grant** *School of Aeronautics and Astronautics, Purdue University **NASA Langley Research Center IGARSS – Vancouver, Canada - July 24-29, 2011 1 Outline • Background – Previous Work – Overview of XM Radio System – Motivation • Objective • Airborne Experiment • Data Processing • Results • Summary and Future Work IGARSS – Vancouver, Canada - July 24-29, 2011 2 Previous Work • Global Navigation Satellite System Reflectometry (GNSS-R) – First demonstration of remote sensing with “signals of opportunity” – Retrieval of ocean surface roughness, wind speed, soil moisture, and ice – 15 years of development: airborne and space (UK-DMC) – GNSS-R enabled by use of known pseudo-random noise (PRN) code • Digital Communication Signals Reflectometry – Expand methods to other “signals of opportunity” – Demonstrated with XM digital radio • Commercial satellite radio system in the US IGARSS – Vancouver, Canada - July 24-29, 2011 3 Motivation • Why Digital Communication Signals? – Multiple frequency bands: Different sensitivity – Higher transmitted power: Better accuracy – Located in geostationary orbit: Fixed geometry • Challenge: – No a priori knowledge of data bits • Hypothesis: – Data bits are long, random, uncorrelated stream • Hypothesis verified using XM digital radio signals (S-band) [Shah, et al, IGARSS 2010] IGARSS – Vancouver, Canada - July 24-29, 2011 4 XM System • Two active geostationary satellites o – Rhythm (115 W) • Elevation: 31.3o • Azimuth: 234.4o o – Blues (85 W) • Elevation: 41.6o • Azimuth: 196.4o IGARSS – Vancouver, Canada - July 24-29, 2011 5 Objective • Quantify retrieval anisotropy between two satellites at different azimuth • Examine potential to retrieve wind direction from this effect IGARSS – Vancouver, Canada - July 24-29, 2011 6 Airborne Experiment IGARSS – Vancouver, Canada - July 24-29, 2011 7 Waveforms • Altitude of the aircraft: 3,471 meters (11,400 feet) • Cross-correlation of direct and reflected signals Flight Result, Fs = 8MHz, Altitude = 3174 meters X: 12.13 Y: 1 1 0.9 X: 17.13 Y: 1 Satellite "Blues" Satellite "Rhythm" 0.8 |Y(ο΄k,0)| 2 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0 5 10 15 Lags[οsec] 20 • Sampling Frequency − 8MHz • Coherent Integration − 10ms • Incoherent Integration − 1sec IGARSS – Vancouver, Canada - July 24-29, 2011 8 Data Processing • Two-step estimation process [Garrison 2003] • First step: – Isotropic normal PDF assumed – Nonlinear least squares estimation π½ππ πΏπΊπ½ = πππ ππ , 0 2 − ππ ππ, , 0; πΏπΊπ½ 2 2 π πΏπΊπ½ = π 2 πΌππππ , πππ , π0ππ π 2 πΌππππ = Mean Square Slope (MSS) πππ = Scale factor (remove variation in signal power) π0ππ = Delay offset (adjust small uncertainties in delay) – Independent estimate for each satellite IGARSS – Vancouver, Canada - July 24-29, 2011 9 Data Processing • Chesapeake Lighthouse (CHLV2): 7.5 m/s (MSS = 0.0010) Flight Estimation, Elevation = 46.3o, Azimuth = 196.4o Flight Estimation, Elevation = 31.3o, Azimuth = 234.4o 0.8 1 0.7 0.8 0.6 0.6 k |Y( ο΄ ,0)|2 k |Y( ο΄ ,0)|2 0.5 0.4 0.3 0.2 0.4 0.2 0.1 0 0 12 13 14 Lags[οsec] 15 16 Rhythm: 0.0076 (6 m/s) 17 16 17 18 19 20 Lags[οsec] 21 22 23 Blues: 0.0098 (7.2 m/s) IGARSS – Vancouver, Canada - July 24-29, 2011 10 Data Processing • Second Step: – 2-D normal slope PDF – Model fit to both satellites simultaneously – Isotropic MSS su2+sc2 fixed to average from first step – Cross-/up-wind ratio (sc/su) fixed to 0.85 – Principal axis α of PDF varied to minimize residuals π½ πΆ = πππ ππ , 0 ππ π ππ ππ, , 0; πΆ 2 2 − ππ ππ, , 0; πΆ 2 2 = π π 2 ππ − π0 , 0; π 2 π’ , π 2 π , πΌ – Wind direction with respect to North ππ = ππ§1,2 − πΌ IGARSS – Vancouver, Canada - July 24-29, 2011 11 Results • Minimum residual found at θW = 57o 4.2815 x 10 Sum of residuals from the two satellites 8 4.281 4.2805 Residuals 4.28 4.2795 4.279 4.2785 4.278 4.2775 4.277 0 20 40 60 80 100 120 140 160 180 Wind Direction from the North, in degrees IGARSS – Vancouver, Canada - July 24-29, 2011 12 Results • CHLV2 reported that the wind direction was 28o • Discrepancy can be due to: – CHLV2 & measurement location separated by 80km • Closest Buoy (44014) not reporting data – Azimuth separation between satellites only 38o - may give reduced sensitivity IGARSS – Vancouver, Canada - July 24-29, 2011 13 Summary and Future Work • Summary – Anisotropy gives equivalent wind speed difference of 1.2m/s – Wind direction may contribute to this effect – Difference between principal axis of wind speed was 29o • Future Work – Single model fit to both satellites data – Find better surface truth values: • Model runs at measurement location IGARSS – Vancouver, Canada - July 24-29, 2011 14 Thank You! IGARSS – Vancouver, Canada - July 24-29, 2011 15 References J.L. Garrison, A. Komjathy, V.U. Zavorotny, and S.J. Katzberg, “Wind speed measurement using forward scattered GPS signals,” IEEE Transactions on Geoscience and Remote Sensing, vol. 40(1), pp. 50–65, 2002. J.L. Garrison, S.J. Katzberg, and M.I. Hill, “Effect of sea roughness on bistatically scattered range coded signals from the Global Positioning System,” Geophys. Res. Lett, vol. 25(13), pp. 2257–2260, 1998. E. Cardellach and A. Rius, “A new technique to sense non-Gaussian features of the sea surface from L-band bi-static GNSS reflections,” Remote Sensing of Environment, vol. 112, no. 6, pp. 2927 – 2937, 2008. R. Shah, J.L. Garrison, M.S. Grant, and S.J. Katzberg, Analysis of correlation properties of digital satellite signals and their applicability in bistatic remote sensing,” Proceedings of the 2010 IEEE International Geoscience and Remote Sensing Symposium, pp. 4114–4117, July 2010. J.L. Garrison, “Anisotropy in reflected GPS measurements of ocean winds,” Proceedings of the 2003 IEEE International Geoscience and Remote Sensing Symposium, pp. 4480–4482, July 2003. IGARSS – Vancouver, Canada - July 24-29, 2011 16 BACKUP AND EXTRAS IGARSS – Vancouver, Canada - July 24-29, 2011 17 Previous Work • Waveform generated by cross-correlating ocean-reflected signals with locally generated pseudorandom code was used • Methods used: – Matched Filters (Garrison, et al 1998) – Nonlinear least squares parameter estimation (Garrison, et al 2002) – Discretized approximation of the full-slope PDF (Caedellach, et al 2008) IGARSS – Vancouver, Canada - July 24-29, 2011 18 Glistening Zone • Rhythm: Semi-major = 4.76km, Semi-minor = 2.47km • Blues: Semi-major = 5.40km, Semi-minor = 2.80km Glistening Zone 3 Rhythm Blues 2 Y [km] 1 0 -1 -2 -3 0 2 4 6 8 10 12 14 X [km] IGARSS – Vancouver, CANADA- July 21-24, 2010 19 Airborne Experiment: Geometry • Experiment conducted: 02-July-2010 in Piper Navajo • Experiment time period: 07:51AM EDT - 09:19AM EDT IGARSS – Vancouver, Canada - July 24-29, 2011 20