She gas-slurry transport bed is a unique operation where the upward flow of a liquid-solid suspension is contacted with the concurrent up-flow of a reacting gas. Such an operation is exemplified by the main reactor and the preheater in a coal liquefaction process (Onozaki et al., 2000). The chemical absorption associated with reactant or product solids suspension for environmental protection use, the UASB unaerobic process using a suspended granular bed of self-coagulated microorganisms for treating wastewater from a food processing factory and the suspension electrolysis of metals are other industrial applications of the gas-slurry transport bed operation (e.g., Fan, 1989;Deckwer, 1992). The heat and mass transfer characteristics in the gas-slurry transport bed are important parameter in designing such a reactor.In the gas-liquid-solid fluidized beds where rather coarser particles are suspended in an expanded stationary bed, the wall-to-bed heat transfer coefficients were measured and correlated by several investigators (Muroyama et al., 2001b). So far several generalized correlation methods have been proposed for the heat and mass transfer coefficients in the gas-liquid-solid fluidized bed. Kato et al. (1981) measured the wall heat transfer coefficient using a short wall heater and correlated the data using a dimensionless empirical correlation. A similar approach was also employed by Kato et al. (1984a,b) and Kang et al. (1985) for correlating the immersed cylinder-to-bed heat transfer data in the three-phase fluidized bed. Muroyama et al. (1986a, b) employed the so called Colburn j-factor approach, that measured the apparent wall heat transfer coefficient excluding the effect of the interior radial heat transfer resistance and correlated the heat transfer coefficient in terms of the modified j-factor and the modified Reynolds number, correcting for the effect of bed expansion on the effective liquid velocity and the spatial arrangement of the particles. Meanwhile, Yasunishi et al. (1988) measured and correlated the wall-to-liquid mass transfer coefficient in the three-phase fluidized beds using the limiting current method. They correlated the mass transfer coefficient in a unified dimensionless formula in terms of the Sherwood number, the Schmidt number and the specific power group including the energy dissipation rate per unit mass of liquid. They indicated the presence of an analogy between the wall-to-liquid mass transfer and heat transfer in the three-phase fluidized bed. Muroyama et al. (2001a) measured the cylinder surface-to-liquid mass transfer coefficients for the vertically and horizontally arranged electrodes using the limiting current method and correlated the data in the same way as employed by Yasunishi et al. (1988). Muroyama et al. (2001b) In the present study we measured the immersed vertical cylinder surface-to-slurry heat transfer coefficient in the liquid-solid and gas-slurry (three-phase) transport beds at controlled solid concentrations. The slurry contained 0.1 mm inert glass beads...