C. Mastenbroek et al., EXPERIMENTAL-EVIDENCE OF THE RAPID DISTORTION OF TURBULENCE IN THE AIR-FLOW OVER WATER-WAVES, Journal of Fluid Mechanics, 318, 1996, pp. 273-302
Detailed observations of the air flow velocity, pressure and Reynolds
stresses above water waves in a wave flume are presented. The static p
ressure fluctuations induced by the waves are observed following a new
procedure that eliminates acoustical contamination by the wave maker.
The measurements are analysed by comparing them with numerical simula
tions of the air flow over waves. In these numerical simulations the s
ensitivity to the choice of turbulence closure is studied. We consider
ed both first-order turbulence closure schemes based on the eddy visco
sity concept, and a second-order Reynolds stress model. The comparison
shows that turbulence closure schemes based on the eddy viscosity con
cept overestimate the modulation of the Reynolds stress in a significa
nt part of the vertical domain. When an eddy viscosity closure is used
, the overestimated modulation of the Reynolds stress gives a signific
ant contribution to the wave growth rate. Our results confirm the conc
lusions Belcher & Hunt reached on the basis of the rapid distortion th
eory. The ratio of the wind speed to the phase speed of the paddle wav
e in the experiment varies between 3 and 6. The observed amplitudes of
the velocity and pressure perturbation are in excellent agreement wit
h the simulations. Comparison of the observed phases of the pressure a
nd velocity perturbations shows that the numerical model underpredicts
the downwind phase shift of the undulating flow. The sheltering coeff
icients for the flow over hills and the growth rates of waves that are
slow compared to the wind calculated with the Reynolds stress model a
re in excellent agreement with the analytical model of Belcher & Hunt.
Extending the calculations to fast waves, we find that the energy flu
x to waves travelling almost as fast as the wind is increased on going
from the mixing length turbulence closure to the Reynolds stress mode
l.