equilibrated is determined, starting with a time-dependent asymptotic field equation for (Rτ)−
1− 1= ε→ 0, where R> 1 is the T/S density ratio and τ= KS/KT< 1 is the molecular diffusivity
ratio. A mode truncation of that equation yields an ODE which shows that the fastest growing
finger mode transfers energy to two 'slave'modes with relatively small vertical scale; the
finger mode thereby attains a statistically steady amplitude. The results for τ= 1/3 are …