STUDIES OF FINITE AMPLITUDE SHEAR WAVE INSTABILITIES. James T. Kirby. Center for Applied Coastal Research. University of Delaware.

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STUDIES OF FINITE AMPLITUDE SHEAR WAVE INSTABILITIES James T. Kirby Center for Applied Coastal Research University of Delaware Newark, DE 19716 phone: (32) 831-2438, fax: (32) 831-1228, email: kirby@coastal.udel.edu Award# N14-94-1-214 LONG-TERM GOALS My long-term goal is to develop numerical codes which are applicable to the full range of low-frequency surfzone motions, to test and rene these codes using results from eld measurement programs, and to apply these codes to the prediction and characterization of uid motions and resulting sediment transport and evolution of beach morphology. OBJECTIVES The scientic objective of this study is to gain an understanding of various features of the low frequency nearshore current climate, including: 1. The long term evolution and dynamics of shear waves. 2. The eect of interaction and competition between several unstable wavenumber modes of nite amplitude shear waves. 3. The dynamics of edge waves in an environment where the underlying longshore current structure is strongly modied by the presence of shear waves. 4. The eect of organized forcing of the shear waves by the incident waves. The motions being studied can provide a sizeable portion of the total energy content in inner surfzone motions, and thus have a (presently not understood) impact on sediment transport and the evolution of beach morphology. We seek to eventually address these issues using the information about the hydrodynamic environment obtained from the present study. APPROACH We have developed a numerical code with the objective of studying the motions and combinations of motions described above. This code has been used to study the long-time evolution of shear waves over realistic beach topographies with and without longshore bars. We have investigated the relative importance of bottom friction and turbulent and dispersive lateral mixing mechanisms in controlling the growth of shear waves, and we have, in turn, investigated the relative importance of small-scale lateral mixing and shear wave-induced Reynolds stresses in determining the distribution of wave-induced longshore current. The code will be further utilized to investigate the eects on shear wave evolution caused by spatial and temporal inhomogeneity of both driving forces and bottom topography. Finally, the model is being extended to allow for the computation of an 1

Report Documentation Page Form Approved OMB No. 74-188 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 124, Arlington VA 2222-432. 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 3 SEP 1997 2. REPORT TYPE 3. DATES COVERED --1997 to --1997 4. TITLE AND SUBTITLE Studies of Finite Amplitude Shear Wave Instabilities 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) University of Delaware,Center for Applied Coastal Research,Newark,DE,19716 8. PERFORMING ORGANIZATION REPORT NUMBER 9. SPONSORING/MONITORING AGENCY NAME(S) AND ADDRESS(ES) 1. SPONSOR/MONITOR S ACRONYM(S) 12. DISTRIBUTION/AVAILABILITY STATEMENT Approved for public release; distribution unlimited 13. SUPPLEMENTARY NOTES 14. ABSTRACT 11. SPONSOR/MONITOR S REPORT NUMBER(S) 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 5 19a. NAME OF RESPONSIBLE PERSON Standard Form 298 (Rev. 8-98) Prescribed by ANSI Std Z39-18

evolving bottom. WORK COMPLETED A model of the nonlinear shallow water equations with additional bottom friction and forcing terms has been developed. The model is robust and the numerical code has been rened in a number of ways to pursue numerical experiments simulating various types of low frequency motions in the surf zone as well as in the swash zone. The model has been extensively tested and has been applied to the generation of subharmonic edge waves and their growth to nite amplitude ( Ozkan-Haller and Kirby, 1997a). The model was used to analyze the dynamics of shear waves in the absence of other low frequency motions. For this purpose we rst simulated shear instabilities of the longshore current on a plane beach ( Ozkan and Kirby, 1995). Studies were also carried out examining if shear instabilities of the longshore current account for the low frequency energy observed at the Superduck experiment ( Ozkan-Haller and Kirby, 1996). The low frequency climate at Superduck was examined by attempting to identify the combination of bottom friction and mixing coecients which led to a ow regime that best reproduced the observations ( Ozkan-Haller and Kirby, 1997b). RESULTS Studies of shear instabilities on a plane beach have produced results which are in agreement with independent results by Allen, Newberger and Holman (J. Fluid Mech, 1996) who utilized a rigid lid model. It was shown that the long term evolution of instabilities in the longshore current is strongly dominated by subharmonic transitions. These transitions were analyzed in detail ( Ozkan-Haller, 1997). We found that the transitions occur in the form of vortex collisions where aweaker vortex structure catches up and collides with a slower more energetic vortex in front of it. During the collision of the vortices, there appears to be an exchange of identities of trailing and leading events, much as in the elastic collision of shallow water solitons. After the collision, most of the energy is transferred to the initially weaker trailing vortex and a subsequent reduction in the number of large vortices is evident. The resulting ow structures are longshore progressive and exhibit strong oshore directed velocities. These results are possibly suggestive ofamechanism for the formation of migrating rip currents. Since it is suspected that rip current motions may beintensied by the distortion to the incident wave eld caused by wave-current interaction effects, we are exploring the inclusion of this distortion in the forcing terms in the numerical model. Several cases using measured bottom bathymetry and wave heights from the Superduck eld study have also been studied. Bottom friction as well as momentum mixing due to turbulence and depth variations in the currents are taken into account. A friction coecient c f and a mixing coecient M control the 2

f (Hz) f (Hz) nature of the simulated motions. We deduce a realistic range of values for c f and M from measurements. Decreasing c f within that range results in more energetic shear instabilities with higher propagation speeds. At present, we use the predicted propagation speed of shear waves as the criterion for determining a \best" friction coecient (see Figure 1), and then use the predicted maximum longshore current velocity asaverication of this procedure. The shear instabilities induce signicant momentum mixing in the surf zone and alter the mean longshore current prole. The current prole before the instabilities are initiated along with the nal mean current prole are shown in Figure 2 for one case at Superduck. Also shown are the measured mean currents. It is observed that the nal current prole is not altered by the amount of mixing due to processes other than the instabilities. If more mixing due to turbulence is assumed (higher M), the instabilities are less energetic and the mixing due to the instabilities decreases proportionally to produce the same current prole. In all cases mixing due to the instabilities is seen to dominate over other mixing mechanisms. However, the reason for the apparent balance between the various mixing mechanisms and the resulting insensitive longshore current prole is not understood and deserves further investigation. Vortex interactions of the type observed for the simpler case of a sloping bottom are also present for the cases involving the barred Superduck bathymetry. Snapshots of the vorticity eld (Figure 3) show the complicated nature of the motions. Vortex pairs propagate in the longshore direction y, interact, occasionally merge and are shed oshore..3.25 f =:83k, :27 Data.3.25 f =:85k, :33 c f =.35 M =.25.2.15.2.15.1.1.5.5.2.2 k (1/m).2.2 k (1/m) Figure 1: Frequency-cyclic longshore wavenumber spectra S(f;k) (m 3 /s) for longshore velocities from measurements on October 16. The equation for the dispersion line (dashed) is noted. 3

IMPACT/APPLICATIONS This study has shed light on the processes that are important in the low frequency range of the energy spectrum, such as interactions between low frequency waves and response of the low frequency environment to external forcing. As shear waves have an important eect on the velocity structure around the breaker line they are also a plausible explanation for oshore mixing. As a result of this study the magnitude of this eect can be assessed and the general understanding of nearshore circulation and mixing patterns can be advanced. This study can also serve as a benchmark for other studies that are not restricted to low frequency motions, but where the low frequency motions are embedded in higher frequency oscillations, making the processes dicult to identify. TRANSITIONS The model code developed here is being used in an ONR-funded study of the inversion of SAR images of the water surface to determine bottom bathymetry (with R. A. Dalrymple, Delaware), in conjunction with a much more numerically intensive Boussinesq wave model. The model and results also form the basis of further proposed work on edge wave and shear waveinteractions (Putrevu, Kirby and Oltman-Shay, NSF) and on the characterization of nearshore motion using coherent structure analysis (Kirby, ONR). REFERENCES Ozkan, H. T. and Kirby, J. T. 1995. Finite amplitude shear wave instabilities. Proceedings of Coastal Dynamics 1995, Gdansk, 465-476. Ozkan-Haller, H. T. and Kirby, J. T. 1996. Numerical study of low frequency surf zone motions. Proceedings of 25th International Conference on Coastal Engineering, Orlando, 1361-1374. Ozkan-Haller, H.T. 1997. Nonlinear Evolution of shear instabilities of the longshore current. Ph.D. dissertation, University of Delaware. Ozkan-Haller, H. T. and Kirby, J. T. 1997a. A Fourier-Chebyshev collocation method for the shallow water equations including shoreline runup. Applied Ocean Research, 19, 21-34. Ozkan-Haller, H. T. and Kirby, J. T. 1997b. Shear instabilities of longshore currents: Flow characteristics and momentum mixing during Superduck. Proceedings of Coastal Dynamics 1997, Plymouth, in press. 4

hvi (m/s) 2 1.5 1.5, V. hvi 5 1 15 2 25 3 35 4 45 5 55 Figure 2: Time and longshore-averaged longshore currents hvi for October 16 for c f =:35 and M = (solid), M =:25 (dashed), M =:5 (dash-dotted) and sled data (o). Also shown is the mean current in the absence of shear instabilities V for c f =:35 and M =:5 (dotted). 25 t t+5 min t+1 min.4.3 2.2 15.1 y (m) 1.1 5.2.3 5 5 5.4 Figure 3: Snapshots of contour plots of vorticity q (1/s) at 5 minute intervals for c f =:35 and M=.25. 5