A mathematical model to describe a circulating fluidized-bed combustor is presented. A modified two-phase model which was used in the bubbling fluidized-bed combustor is considered to simulate the dense zone of the bottom section. For the upper section of the bed the momentum and energy-balance equa
Numerical solution of a two-dimensional fluidized bed model
β Scribed by I. Christie; G. H. Ganser; J. W. Wilder
- Publisher
- John Wiley and Sons
- Year
- 1998
- Tongue
- English
- Weight
- 200 KB
- Volume
- 28
- Category
- Article
- ISSN
- 0271-2091
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β¦ Synopsis
The numerical solution of a model describing a two-dimensional fluidized bed is considered. The model takes the form of a hyperbolic system of conservation laws with source term, coupled with an elliptic equation for determining a streamfunction. Operator splitting is used to produce homogeneous one-dimensional hyperbolic systems and ordinary differential equations involving the source term. The one-dimensional hyperbolic problems are solved using Roe's method with the addition of an entropy fix. The numerical procedure is second-order in time and first-order in space. Second-order-accuracy in space is obtained using flux limiting techniques. Numerical experiments which show the development of bubbles in the bed are presented. The familiar kidney-shaped bubble, observed experimentally, is found when using the method which is second-order in space. On the same mesh, the first-order method produces bubbles which are no longer kidney-shaped.
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The one-dimensional dispersion model under the assumption that the fluid is completely mixed in the radial direction is generally used to describe turbulent mixing in apparatus with axial flow. With increasing apparatus diameter, however, this assumption becomes less correct and it becomes necessary
Knowledge of bed expansions is important in the design and operation of gas-solid fluidized beds. This paper presents a study on the estimation of expanded bed height in a large three-dimensional gas-fluidized bed with a square section of 0)61;0)61 m. All experiments were performed at the freely bub