Natural convection in wide spherical shells of aspect ratio β = 1 changes in fundamental ways, when the Rayleigh number Ra reaches critical values. For low Ra the convection is steady and axisymmetric, but above a critical value it becomes timedependent, with plumes dripping of the 'south pole' periodically. At higher Ra these still two-dimensional convective pulses become irregular in time, the transition occuring with period-doubling bifurcation. Our numerical investigations of the flow show this transition scheme from steady to periodic to chaotic behaviour to be independent for Prandtl numbers P r greater than 100. For decreasing P r down to 6 the steady, axisymmetric basic state is observed up to higher and higher Ra. For β = 1 the onset of periodicity appears at higher Ra, too. Small gap-width reveal a crescent-eddy type flow, wide gap-width reveal a varied kidney-shaped eddy type.