Tomographic imaging of a conical fluidized bed of dry pharmaceutical granule

作者：Wiens Jason; Pugsley Todd^*

来源：Powder Technology, 2006, 169(1): 49-59.

DOI：10.1016/j.powtec.2006.07.022

• fluidization
• conical bed
• electrical capacitance tomography
• hydrodynamics
• bubbling
• turbulent

Hydrodynamics in a conical fluidized bed were studied using electrical capacitance tomography (ECT) for a bimodal and mono-disperse particle size distribution (PSD) of dry pharmaceutical granule. The bimodal PSD exhibited a continuous distribution with modes at 168 and 1288 pin and contained approximately 46% Geldart A, 32% Geldart B and 22% Geldart D particles by mass. The mono-disperse PSD had a mean particle size of 237 gin and contained approximately 71% Geldart A, 27% Geldart B, and 2% Geldart C particles by mass. The granule particle density was 830 kg/m(3). Experiments were conducted at a static bed height of 0.16 in for gas superficial velocities ranging from 0.25 to 2.50 m/s for the mono-disperse PSD, and from 0.50 to 3.00 m/s for the bimodal PSD. These gas velocities covered both the bubbling and turbulent fluidization regimes. An 'M'-shaped time-averaged radial voidage profile appeared upon transition from bubbling to turbulent fluidization. The 'M'-shaped voidage profile was characterized by a dense region near the wall of the fluidized bed with decreasing solids concentration towards the centre. An increased solids concentration was observed in the middle of the bed. Frame-by-frame analysis of the images showed two predominant bubble types: spherical bubbles with particle penetration in the nose which created a core of particles that extended into, but not through, the bubble; and spherical bubbles. Penetrated bubbles, responsible for the 'M' profile, were a precursor to bubble splitting; which became increasingly prevalent in the turbulent regime.

• 出版日期2006-10-24