Determination of Nearshore Wave Conditions and Bathymetry from X-Band Radar Systems

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Determination of Nearshore Wave Conditions and Bathymetry from X-Band Radar Systems Okey G. Nwogu Dept. of Naval Architecture and Marine Engineering University of Michigan Ann Arbor, MI 48109 Phone: (734) 764-0494 Fax: (734) 936-8820 E-mail: onwogu@engin.umich.edu Paul S. Bell Proudman Oceanographic Laboratory Birkenhead CH43 7RA United Kingdom Phone: (44) 151 653-1570 Fax: (44) 151 653-6269 E-mail: psb@pol.ac.uk Award Number: N00014-03-1-0442 http://www-personal.engin.umich.edu/~onwogu/ LONG-TERM GOALS The long-term goal of this research project is to improve our capability to use X-band marine radars to routinely measure waves, currents and bathymetry in coastal regions. OBJECTIVES The scientific objectives of this study are: 1. investigate the imaging mechanisms of X-band radar systems in shallow coastal waters where nonlinear wave steepening, infragravity waves, wave breaking and breaking-induced currents can affect the radar backscatter signal 2. apply high-resolution spectral analysis techniques to the estimation of directional wave spectra from X-band radar images. 3. develop improved techniques for estimating the bottom topography from X-band radar images of the sea surface in shallow water regions with highly nonlinear waves and/or strong currents. APPROACH Proudman Oceanographic Laboratory (POL) deployed an X-band (9.8GHz, 3cm wavelength) marine radar during the European COAST3D field experiments in Teignmouth, UK. The study site is a complex three-dimensional tidal inlet. A sequence of 64 radar images was collected at time interval of 2.25s every hour. Although realistic-looking wave patterns are observed in the radar images, it is still unclear how the radar image intensities are related to the sea surface elevation. Marine radars rely upon the scattering of incident electromagnetic waves by the ocean surface to detect ocean waves. Since the 3-cm wavelength of the X-band radar is much smaller than the typical wavelength of gravity waves, it 1

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 30 SEP 2004 2. REPORT TYPE 3. DATES COVERED 00-00-2004 to 00-00-2004 4. TITLE AND SUBTITLE Determination of Nearshore Wave Conditions and Bathymetry from X-Band Radar Systems 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) Dept. of Naval Architecture and Marine Engineering,,University of Michigan,,Ann Arbor,,MI,48109 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 11. SPONSOR/MONITOR S REPORT NUMBER(S) 14. ABSTRACT The long-term goal of this research project is to improve our capability to use X-band marine radars to routinely measure waves, currents and bathymetry in coastal regions. 15. SUBJECT TERMS 16. SECURITY CLASSIFICATION OF: 17. LIMITATION OF ABSTRACT a. REPORT unclassified b. ABSTRACT unclassified c. THIS PAGE unclassified Same as Report (SAR) 18. NUMBER OF PAGES 6 19a. NAME OF RESPONSIBLE PERSON Standard Form 298 (Rev. 8-98) Prescribed by ANSI Std Z39-18

is actually the modulation of the radar backscatter by longer gravity waves that governs the appearance of ocean wave patterns in radar images. In shallow coastal waters, the imaging process is further complicated by several factors including nonlinear wave steepening/shadowing, wave breaking, low frequency fluctuations of the mean water level (infragravity waves), and wave-induced currents. Our approach is to use a time-dependent nonlinear wave propagation model to elucidate the nature of the imaging mechanism of X-band radar systems in nearshore regions. The numerical model is based on a finite difference solution of a fully nonlinear set of Boussinesq-type equations (Nwogu, 1993; Nwogu and Demirbilek, 2001). The governing equations are uniformly valid from deep to shallow water and can simulate most of the phenomena of interest in the nearshore zone including shoaling, refraction, diffraction, reflection, bottom friction, nonlinear wave-wave interactions, wave breaking, wave-induced currents and wave-current interaction. The Boussinesq model is used to simulate the wave conditions that were observed during the COAST3D experiments. Numerical model predictions are compared to data from in-situ gauges. Cross-spectral analysis techniques are used to determine the transfer function and coherence between the predicted wave field and the radar backscatter intensities. We then investigate the variation of the transfer function with factors such as wind speed, wave propagation direction, wave height, distance from antenna, etc. 3-D FFT techniques are commonly used to estimate the normalized directional wave spectra from X- band radars (e.g. Young et al., 1985). The 3-D FFT analysis technique implicitly assumes that the wave conditions are stationary and homogenous over the analysis area. This assumption is typically valid in radar image domain sizes of the order of 2km x 2km in deep water. However, we are primarily interested in shallow water where the effects of refraction, diffraction, nonlinear wave-wave interaction, wave breaking, and wave current interaction lead to a non-spatially homogenous wave field. To estimate the directional wave spectra, we need to select subregions of the image with locally spatially homogenous conditions. This might involve subdomain sizes of the order of 2-5 wavelengths. Applying standard 3-D FFT techniques to such domain sizes will lead to the smearing of the wave energy in wavenumber space. Spectral analysis methods such as the Maximum Entropy Method (MEM) have been shown to provide high-resolution spectral estimates for short non-cyclic records. Hence, we propose to conduct maximum entropy spectral analysis of subregions of the radar image to compare with the standard FFT analysis method. Directional wave spectra determined from the X-band radar data at the in-situ gauge locations will be compared with the measured directional spectra. Data from X-band marine radars have been used to infer the bathymetry in coastal waters. Since the radars provide a time-varying sequence of images of the sea surface, Bell (1999) used a motiontracking algorithm to determine the wave propagation speeds, wavelengths and directions. A depth inversion algorithm based on linear wave theory was used to estimate the water depths from the phase speeds and wavelengths. Good agreement was generally observed between the inferred and surveyed depths except in regions with strong currents and very shallow water where linear theory breaks down. An improved depth inversion algorithm is being developed based on Boussinesq wave theory. WORK COMPLETED To allow direct time-domain comparisons of numerical model predictions with in-situ gauges, as well as direct comparisons of numerically simulated wave fields with X-band radar images, we modified the Boussinesq model to synthesize multi-directional sea states from the time series of the surface elevation and two components of the horizontal velocity at a gauge location close to the incident wave 2

boundary. The phases of the different frequency components are no longer selected at random and the directions are uniquely determined from the amplitudes of the velocity components. We have run the Boussinesq model for several incident wave conditions that occurred during the COAST3D Teignmouth experiments. The predicted directional wave spectra at several gauge locations have been compared to the measured data. We have also implemented a 3-D FFT analysis algorithm to estimate directional wave spectra from X-band radar data. We have also implemented two highresolution spectral analysis algorithms based on the maximum entropy and maximum likelihood methods. We initially developed a nonlinear depth-inversion algorithm based on Boussinesq theory. However, the scheme could not successfully be applied to a sequence of radar images due to the amount of noise in the images and lack of one-to-one correlation between the radar intensity and sea surface elevation. We thus developed an improved linear depth inversion algorithm that utilizes highresolution wavenumber estimates from the maximum likelihood method. RESULTS We initially present results of the Boussinesq model simulations for the COAST3D Teignmouth experiments. Numerical simulations were carried out for a storm event that occurred on 11/12/99 at 06:00GMT. The incident wave climate at Gauge #3a had significant wave height H s = 1.6m, and peak period T p = 7.5s. The boundary conditions for the numerical model were synthesized to match the surface elevation and two components of the horizontal velocity at Gauge #3a close to the offshore boundary. Figure 1 shows the observed radar image of the sea surface while Figure 2 shows the wave field predicted by the Boussinesq model. In general, the signal to noise ratio of the radar image decreased with increasing distance from the antenna. Figure 1. X-Band Radar Image of Sea Surface. Figure 2. Simulated Wave Field with Boussinesq Model 3

Elevation (m) 0.6 0.4 0.2 0-0.2 Boussinesq Model X-Band Radar -0.4 0 250 500 750 1000 Distance (m) Figure 3. Comparison of Predicted Sea Surface Elevation with Radar Backscatter Intensity Along a Transect with Shoreline (T=7.5s). Figure 4. Measured Bathymetry Figure 5. Inferred Bathymetry The dominant wave component (T=7.5s) was filtered out from the sequence of radar images and compared to the sea surface elevation prediction from the Boussinesq model along a shorenormal transect (see Figure 3). The normalized radar intensity matched the simulated sea surface elevation reasonably well at distances of 200 m to 500 m from the shoreline. There are however pronounced differences closer to shoreline where the waves are breaking and at distances of O(1km). We intend to 4

use the Boussinesq model to guide development of an improved radar transfer function for nearshore applications. Preliminary comparisons of the measured and inferred bathymetries using the improved depth inversion algorithm are shown in Figures 4 and 5 respectively. The sand banks and navigation channel are well resolved by the inversion algorithm although the inferred depths are still relatively noisy and model performance is poorer in deeper water. We are currently optimizing several parameters in the depth inversion algorithm improve the model-data comparisons. IMPACTS/APPLICATIONS The X-band radar represents a unique and economically affordable tool for the remote observation of coastal regions. It can be used to measure directional wave spectra and circulation patterns in complex three-dimensional coastal inlets and map the underwater topography in areas that are too hazardous for traditional hydrographic survey methods. It is anticipated that this project will lead to the development of several robust algorithms for analyzing the wave field and inferring bottom topography X-band radar images. REFERENCES Bell, P.S. 1999. Shallow water bathymetry derived from an analysis of X-band radar images of waves. Coastal Engineering, 37(3-4), 513-527. Nwogu, O. 1993. Alternative form of Boussinesq equations for nearshore wave propagation. Journal of Waterway, Port, Coastal and Ocean Engineering, ASCE, 119(6), 618-638. Nwogu, O.G. and Demirbilek, Z. 2001. BOUSS-2D: A Boussinesq Wave Model for Coastal Regions and Harbors. Technical Report ERDC/CHL TR-01-25, U.S. Army Engineer Research and Development Center, Vicksburg, MS. Rienecker, M.M., and Fenton, J.D. 1981. A Fourier approximation method for steady water waves. Journal of Fluid Mechanics, 104, 119-137. Young, I.R., Rosenthal, W. and Ziemer, F. 1985. A Three-Dimensional Analysis of Marine Radar Images for the Determination of Ocean Wave Directionality and Surface Currents. Journal of Geophysical Research, 90, 1049-1059. PUBLICATIONS Nwogu, O.G., Bell, P.S., and L. Meadows. 2003. On the Imaging of Nearshore Waves by X-Band Radar Systems. Paper to be presented at the Coastal Engineering Today Conference, Gainesville, FL, October 2003. Nwogu, O. High-Resolution Estimates of Directional Wave Spectra from X-band Marine Radar Images. J. Geophysical Research (in preparation) Nwogu, O. and Bell, P.S. Determination of Nearshore Bottom Topography from X-Band Marine Radars. (in preparation). 5