T he spouted bed technique has proved to be an effective means of contacting relatively coarse particles with a gas (Epstein and Grace, 1997). Spouted beds differ in geometrical confi guration and, for continuous solids feed, in method of feeding the solids. The most conventional and common confi gurations are either conical or cylindrical with a conical base, the function of the cone in the latter being to prevent the occurrence of stagnant solids at the base. Solids feeding methods include gravity feed to the top of the bed, pneumatic conveying by the spouting gas entering the inlet nozzle at the bottom of the bed, and suction feed whereby particles are fed into the bed sideways near the gas inlet using the suction created by the gas jet entering the bed. Fane et al. (1985) were the fi rst to publish on the behaviour of a spouted bed in which the entering gas stream carried the same solids as those being spouted. In their study, the conicalcylindrical bed was connected to a long vertical riser at the bottom. The particles were fed into the riser via a vibratory feeder that allowed independent control of solids and air fl ow rate. They reported that the maximum spoutable bed height, H m , increased with the total solids loading of the entering gas, and their data also showed a decline of minimum spouting velocity, U ms , with increased loading. These results are in accord with