Ventilated oscillatory boundary layers

Abstract : A combination of field and laboratory experiments are made in order to expand our knowledge of naturally occurring oscillatory boundary layers. Chapter 1 describes field observations of the development of wave driven boundary layers at the fluid sediment interface. Under the crest of the wave, this development can be idealized as an identifiable sequence of three parts. The latter parts of this development are never observed to occur under the trough of the wave despite similarities in wave orbital velocity and acceleration. It is proposed that wave induced boundary ventilation, the oscillatory flow through the surface of a permeable bed, may be responsible for this apparent developmental asymmetry. In chapter 2, a laboratory study is presented of ventilated oscillatory boundary layers. These are boundary layers arising from a flow which oscillates parallel to a permeable bed which is subject to oscillating percolation of the same frequency as the bed parallel flow. Measurements of boundary layer velocities, bed stress and turbulent flow properties are presented. It is observed that suction (flow into the bed) enhances the near bed velocities and bed stress while injection (flow out of the bed) leads to a reduction in these quantities. As the ventilated oscillatory boundary layer experiences both these phenomena in one full cycle, the result is a net stress and a net boundary layer velocity in an otherwise symmetric flow. While production of turbulence attributable to injection is enhanced, the finite time required for this to occur leads to greater vertically averaged turbulence in the suction half cycle. Turbulence generated in the suction half cycle is maintained in a compact layer much closer to the bed. These effects appear to hold for Re ranging from 10(100,000) to 10(1,000,000) and for oscillations other than sinusoidal.

[1]  O. E. Tewfik SOME CHARACTERISTICS OF THE TURBULENT BOUNDARY LAYER WITH AIR INJECTION , 1963 .

[2]  F. Anselmet,et al.  Effect of wall suction on bursting in a turbulent boundary layer , 1990 .

[3]  R. Reid,et al.  On the damping of gravity waves over a permeable sea bed , 1957 .

[4]  W. E. Stewart,et al.  HEAT, MASS, AND MOMENTUM TRANSFER FOR FLOW OVER A FLAT PLATE WITH BLOWING OR SUCTION , 1954 .

[5]  R. Davis,et al.  Momentum Transfer for Flow over a Flat Plate with Blowing , 1957 .

[6]  Robert J. Moffat,et al.  The turbulent boundary layer on a porous plate: Experimental skin friction with variable injection and suction , 1969 .

[7]  D. Inman,et al.  Field observations of the fluid‐granular boundary layer under near‐breaking waves , 1992 .

[8]  J. F. A. Sleath,et al.  Turbulent oscillatory flow over rough beds , 1987, Journal of Fluid Mechanics.

[9]  B. Sumer,et al.  Turbulent oscillatory boundary layers at high Reynolds numbers , 1989, Journal of Fluid Mechanics.

[10]  Robert T. Guza,et al.  Elevation and velocity measurements of laboratory shoaling waves , 1981 .

[11]  R. Flick,et al.  TURBULENCE SCALES IN THE SURF AND SWASH , 1991 .

[12]  Steve Elgar,et al.  Observations of bispectra of shoaling surface gravity waves , 1985, Journal of Fluid Mechanics.

[13]  John D. Powell,et al.  A NEW OSCILLATORY FLOW TUNNEL FOR USE IN SEDIMENT TRANSPORT EXPERIMENTS , 1984 .

[14]  P. Liu Mass transport in water waves propagated over a permeable bed , 1977 .

[15]  W. Kays Heat transfer to the transpired turbulent boundary layer , 1972 .

[16]  O. Madsen,et al.  Combined wave and current interaction with a rough bottom , 1979 .

[17]  Fabien Anselmet,et al.  Influence of wall suction on the organized motion in a turbulent boundary layer , 1988, Journal of Fluid Mechanics.

[18]  David A. Huntley,et al.  Continuous measurements of suspended sand concentration in a wave dominated nearshore environment , 1986 .