Steady, nonlinear, penetrative convection in a viscous, incompressible
fluid confined between free horizontal boundaries in two dimensions i
s investigated numerically. For Prandtl numbers sigma less than unity
and for fixed imposed heat flux, the resulting Rayleigh number R is-pr
oportional-to sigma-1 indicating a strong dependence on the Prandtl nu
mber not realised with two-dimensional Rayleigh-Benard calculations. A
t low Prandtl numbers, the convection bifurcates supercritically and l
ess efficient heat transport and different cell geometry are exhibited
, with no ''flywheel'' solution in existence.