Linearly stratified salt solutions of different Prandtl number were subject
ed to turbulent stirring by a horizontally oscillating vertical grid in a c
losed laboratory system. The experimental set-up allowed the independent di
rect measurement of a root mean square turbulent lengthscale L-t, turbulent
diffusivity for mass K-rho, rate of dissipation of turbulent kinetic energ
y epsilon, buoyancy frequency N and viscosity nu, as time and volume averag
ed quantities. The behaviour of both L-t and K-rho, was characterized over
a wide range of the turbulence intensity measure, epsilon/nuN(2), and two r
egimes were identified.
In the more energetic of these regimes (Regime E, where 300 < epsilon /vN(2
) < 10(5)) was found to be a function of nu, kappa and N, whilst K-rho was
a function of v, kappa and (epsilon/nuN(2))(1/3). From these expressions fo
r L-t and K-rho a scaling relation for the root mean square turbulent veloc
ity scale U-t was derived, and this relationship showed good agreement with
direct measurements from other data sets.
In the weaker turbulence regime (Regime W, where 10 < epsilon/nuN(2) < 300)
K-rho was a function of nu, kappa and epsilon/nuN(2).
For 10 < epsilon/nuN(2) < 1000, our directly measured diffusivities, K-rho
are approximately a factor of 2 different to the diffusivity predicted by t
he model of Osborn (1980). For epsilon/nuN(2) > 1000, our measured diffusiv
ities diverge from the model prediction. For example, at epsilon/nuN(2) the
re is at least an order of magnitude difference between the measured and pr
edicted diffusivities.