A computer model for a hot fluidized bed was developed. The large heat transfer M. SYAMLAL and DlMlTRl GIDASPOW Illinois Institute of Technology Department of Chemical Engineering Chicago, IL 60616coefficients characteristic of fluidized beds were computed without an enhancement of heat transfer by turbulence. They agreed with measurements reported by Ozkaynak and Chen (1980) within the accuracy of estimated thermal conductivity of solids.
SCOPEFluidized beds are ideal for gasifying coal due to high rates of heat and mass transfer and solids mobility. Environmental constraints make them also very useful for coal combustion to produce electric power. However, one of the largest concerns when using fluidized beds to commercialize many chemical processes is scale-up. We believe this is due to the absence of an experimentally verified hydrodynamic theory that can describe the complicated transient gas and solid motion in a fluid bed. During the past few years several organizations began to develop hydrodynamic computer models that promise to be predictive in many respects. In the area of gasification a workshop chaired by Ghate and Martin (1982) summarized the models developed by the Systems, Science and Software group (Schneyer et al., 1981) and by the JAYCOR group . For fluidized bed combustion, the model by Adams and Welty (1979) proved to be very useful for explaining heat transfer coefficients from a horizontal tube to a fluidized bed. A cold fluidized bed model developed at Illinois Institute of Technology (IIT) Ettehadieh, 1982) for a twodimensional bed was able to predict void distributions, solids circulation, and bubbling behaviors. A critical test for a fluidized bed hydrodynamic model, is its ability to predict the experimentally observed large heat transfer coefficients.
CONCLUSIONS AND SIGNIFICANCEThe IIT model was extended to a heated fluidized bed. Our results suggest that in a bubbling bed the large heat transfer coefficients can be computed from our hydrodynamic model without the use of any turbulence as used in the model of Klein and Scharff (1982). The model itself computes a transient type behavior caused by the formation of bubbles, their propagation, and eruption at the top of the bed. All the computed variables, the void fraction, the gas and solid velocities, and the temperatures undergo a complex oscillatory behavior.This model should be useful for studying effects of reactor configurations and for making parametric studies for process optimization.