The results of an experimental study carried out to investigate the st
ructure of turbulence near a shear-free density interface are presente
d. The experimental configuration consisted of a two-layer fluid mediu
m in which the lower layer was maintained in a turbulent state by an o
scillating grid. The measurements included the root-mean-square (r.m.s
.) turbulent velocities, wavenumber spectra, dissipation of turbulent
kinetic energy and integral lengthscales. It was found that the introd
uction of a density interface to a turbulent flow can strongly distort
the structure of turbulence near the interface wherein the horizontal
velocity components are amplified and the vertical component is dampe
d. The modification of r.m.s velocities is essentially limited to dist
ances smaller than about an integral lengthscale. Inspection of spectr
a shows that these distortions are felt only at small wavenumbers of t
he order of the integral scale and a range of low-wavenumbers of the i
nertial subrange; the distortions become pronounced as the interface i
s approached. Comparison of the horizontal velocity data with the rapi
d distortion theory (RDT) analyses of Hunt & Graham (1978) and Hunt (1
984) showed a qualitative agreement near the interface and a quantitat
ive agreement away from the interface. On the other hand, the RDT pred
ictions for the vertical component were in general agreement with the
data. The near-interface horizontal velocity data, however, showed qua
ntitative agreement with a model proposed by Hunt (1984) based on nonl
inear vortex dynamics near the interface. The effects due to interfaci
al waves appear to be important for distances less than about 10% of t
he integral lengthscale. As a consequence of the non-zero energy flux
divergence, the introduction of a density interface to oscillating gri
d turbulence increases the rate of dissipation in the turbulent layer
except near the interface, where a sharp drop occurs. The present meas
urements provide useful information on the structure of turbulence in
shear-free boundary layers, such as atmospheric and oceanic convective
boundary layers, thus improving modelling capabilities for such flows
.