Diffusion model for fluidized-bed drying
β Scribed by M. A. Zoglio; W. H. Streng; J. T. Carstensen
- Publisher
- John Wiley and Sons
- Year
- 1975
- Tongue
- English
- Weight
- 477 KB
- Volume
- 64
- Category
- Article
- ISSN
- 0022-3549
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β¦ Synopsis
A sucroselactose-starch granulation was used to study particulate motion and attrition in a fluid bed dryer. There is some classification of material in the dryer as drying proceeds; fine particles are dried faster and become less dense, and the less dry but denser large particles show some (although not great) accumulation tendencies in the lower central area. Unlike countercurrent rotary drying, fluid bed drying cannot be accounted for by water diffusion inside the granule as the rate-limiting step. In its place, a model of external water vapor diffusion is proposed and is supported by vapor4oncentration curves and by the linear dependence of the rate constants on the linear air velocities. The dried granulation exhibits the same trend as does countercurrent dried material in that larger particles have higher moisture contents than do smaller particles. Quantitative relationships between content of moisture and size were developed and are supported by experimental data. The granulation, upon storage, does not equilibrate, indicating that this type of water distribution is a problem in batch process granulations as well as in the earlier reported case of granulations for continuous production. Keyphrases I I Drying-fluid bed dryer, diffusion model, sucroselactose-starch granulation, rate-limiting step, relationships between moisture and size Diffusion-model for fluidized-bed drying, moisture and size relationships, rate-limiting step 0 Fluid bed dryingdiffusion model, moisture and size relationships, ratelimiting step, equations ~
π SIMILAR VOLUMES
A kinetic model is d e v e l o p e d for t h e drying of solids in fluidized b e d s , assuming a falling rate period following a constant rate period. Experimental d a t a obtained using b a t c h a n d continuous single a n d spiral fluidized b e d s are satisfactorily m a t c h e d with t h e ass
Notation a air mass #ow, kg/s A air mass, kg c , c constants C N speci"c heat, kJ/kg K h enthalpy #ow, kJ/s H total enthalpy, kJ H T latent heat of evaporation, kJ/kg J evaporation rate, kg H O/kg dm s k drying rate constant, s\ ΒΈbed depth, m m #ow rate of dry matter, kg/s M dry matter mass, kg ΒΉ te