Abstract

Published theories and observations have shown that dissipation of gravity waves implies frequency downshifting of wave energy. Hence, for wind-waves, the wind energy input to the highest frequencies is of special interest. Here it is shown that this input is vital, because the direct wind energy input obtained by the air-pressure’s work on most gravity waves is slightly less than what the waves need to grow. Further, the wind’s input of the angular momentum that waves need to grow is found to be absent at most gravity wave frequencies. The capillary waves that appear at the surface of the sea when the wind is blowing solve these problems. To demonstrate this, an extension of linear wave theory is established to study possibilities and limitations for transfer of energy and angular momentum from the wind to waves through these frequencies. The theory describes regular, gravity–capillary waves with constant amplitude under laminar conditions. It includes surface tensions, viscosity, gravity and a wind-generated shear current, and shows that these waves—contrary to most gravity waves—receive more energy from the wind than they dissipate and angular momentum they cannot keep. Hence, the problem of the missing input of energy and angular momentum from wind to gravity waves is solved by transfers through the capillary waves. This implies that capillary waves are vital to obtain growing gravity waves.

Highlights

  • When wind-waves grow, capillary waves are usually present on major parts of the surface of the sea

  • The present theory is reduced to an ordinary, linear gravity wave theory where the viscosity is negligible, i.e., to Airy’s wave theory [13]

  • (47) implies, as we saw in Section 2.4, that, if the amplitude is constant, the dynamical air pressure provides no energy input to the waves. It implies that if the waves grow due to W1, the dynamical air pressure supplies exactly the energy needed for free waves to grow in an ideal fluid, a result that is valid for all wave frequencies, as well as for the gravity waves for which we expect that I = 1

Read more

Summary

Introduction

When wind-waves grow, capillary waves are usually present on major parts of the surface of the sea. It should be noted that the increase in momentum due to wind shear stresses does not end up as increasing currents only, and as Stokes drift of the growing gravity waves. It is a possible explanation for why U was not observed as a function of t in [9], and why V = 0. Since U and V may not be exactly constant, approximations are frequently adopted to simplify formulae when it can be done without significant losses of accuracy

Continuity
The Air Pressure at the Surface
Phase Speed and Frequency
The Air Pressure’s Primary Contribution
The Air Pressure’s Second Contribution
Dissipation and Excess Work
Input of Angular Momentum from the Wind
Frequency Downshifting
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call