Sponsor: Office of Naval Research, Coastal Sciences
Student: H. Tuba Özkan-Haller (Ph.D., 1997)
My long-term goal is to develop numerical codes which are applicable to the full range of low-frequency surfzone motions, to test and refine these codes using results from field measurement programs, and to apply these codes to the prediction and characterization of fluid motions and resulting sediment transport and evolution of beach morphology.
The scientific 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 effect of interaction and competition between several unstable
wavenumber modes of finite amplitude shear waves.
3. The dynamics of edge waves in an environment where the underlying
longshore current structure is strongly modified by the presence of shear
waves.
4. The effect 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.
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 effects 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 evolving bottom.
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 refined 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 finite
amplitude (Özkan-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 first simulated shear instabilities of the longshore current on a plane
beach (Özkan 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 (Özkan-Haller and Kirby, 1996).
The low frequency climate at Superduck was examined by attempting to
identify the combination of bottom friction and mixing coefficients which
led to a flow regime that best reproduced the observations
(Özkan-Haller and Kirby, 1997b).
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 (Özkan-Haller, 1997). We found that the
transitions occur in the form of vortex collisions where a weaker
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 flow
structures are longshore progressive and exhibit strong offshore
directed velocities. These results are possibly suggestive of a
mechanism for the formation of migrating rip currents. Since it is
suspected that rip current motions may be intensified by the distortion
to the incident wave field 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 field 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 coefficient $c_f$ and
a mixing coefficient $M$ control the 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 coefficient (see Figure 1), and then use the predicted maximum
longshore current velocity as a verification of this procedure.
The
shear instabilities induce significant momentum mixing in the surf zone
and alter the mean longshore current profile. The current profile
before the instabilities are initiated along with the final mean
current profile are shown in Figure 2 for one case at Superduck.
Also shown are the measured mean
currents. It is observed that the final current profile 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
profile. 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 profile 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 field (Figure 3) show
the complicated nature of the motions. Vortex pairs propagate in the
longshore direction $y$, interact, occasionally merge and are shed
offshore.
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