Local gas velocity measurements were conducted utilizing a Pitot tube in two small‐scale (Dc = 150 mm, γ = 30°, 60°) and one large‐scale (Dc = 250 mm, γ = 66°) conical spouted beds. Three different types of particles, zirconia (...
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https://www.riss.kr/link?id=O111402820
2021년
-
0008-4034
1939-019X
SCI;SCIE;SCOPUS
학술저널
1607-1615 [※수록면이 p5 이하이면, Review, Columns, Editor's Note, Abstract 등일 경우가 있습니다.]
0
상세조회0
다운로드다국어 초록 (Multilingual Abstract)
Local gas velocity measurements were conducted utilizing a Pitot tube in two small‐scale (Dc = 150 mm, γ = 30°, 60°) and one large‐scale (Dc = 250 mm, γ = 66°) conical spouted beds. Three different types of particles, zirconia (...
Local gas velocity measurements were conducted utilizing a Pitot tube in two small‐scale (Dc = 150 mm, γ = 30°, 60°) and one large‐scale (Dc = 250 mm, γ = 66°) conical spouted beds. Three different types of particles, zirconia (ρp = 6050 kg/m3), zirconia‐toughened alumina (ρp = 3700 kg/m3), and glass beads (ρp = 2460 kg/m3), were used in the experiments. Careful calibration of the Pitot tube for determination of gas velocities in the annulus section was carried out in a separate, loosely packed‐bed set‐up, which represents the flow conditions in the annulus section of the spouted bed. Solids hold‐up profiles were used to calculate the superficial gas velocities and determine the amount of air flowing through the spout, interface, and annulus. Effects of axial position, conical angle, bed size, and particle density on gas velocity profiles were investigated. It is shown that the amount of air flow through the annulus increases as the axial distance and particle density increases; however, it decreases with increasing cone angle. Dispersion of the gas into the annulus is found to be significantly higher in the large‐scale unit than the small‐scale unit.
Radial profile of interstitial velocity for zirconia particles in the: A, spout and interface regions, and B, annulus region (dp = 1 mm, γ = 60°, Hb = 100 mm, U0 = 1.25Ums).