Hydrodynamics and steel tube wastage in a fluidized bed at elevated temperature

被引:21
作者
Johansson, K
Norling, R
Hjörnhede, A
Almstedt, AE [1 ]
Johnsson, F
Nylund, A
机构
[1] Chalmers Univ Technol, Dept Thermo & Fluid Dynam, SE-41296 Gothenburg, Sweden
[2] Chalmers Univ Technol, Dept Mat Sci & Engn, SE-41296 Gothenburg, Sweden
[3] Chalmers Univ Technol, Dept Energy Convers, SE-41296 Gothenburg, Sweden
关键词
fluidization; erosion; fluidized bed combustion; multiphase flow; energy; environment;
D O I
10.1016/j.ces.2003.09.027
中图分类号
TQ [化学工业];
学科分类号
0817 ;
摘要
Hydrodynamic measurements were made in a bubbling fluidized bed operated at 550degreesC at three different excess gas velocities (0.15, 0.40 and 0.75 m/s). The bed has a cross-sectional area of 0.2 m x 0.3 m with an immersed tube bank consisting of 59 horizontal stainless steel tubes (AISI 304L), 21 of which are exchangeable, thus allowing erosion studies. Capacitance probe analysis was used to determine the mean bubble rise velocity, the mean bubble frequency, the mean pierced bubble length, the mean bubble volume fraction and the mean visible bubble flow rate. Tube wastage was calculated from roundness profiles obtained by stylus profilometry. A redistribution of the bubble flow towards the center of the bed occurs when the excess gas velocity is increased. Measurements along a target tube, situated next to the capacitance probe, usually show greater material wastage at the central part of the tube, since the mean bubble rise velocity and the mean visible bubble flow rate are higher there. It is suggested that the greater material degradation is also an effect of the through-flow of a particle-transporting gas stream in the bubbles. With increasing height above the distributor plate the circumferential wastage profiles for the lowest excess gas velocity show a gradual change from an erosion pattern with one maximum (Type B behavior) to a pattern with two maxima (Type A behavior). Power spectral density distributions of the fluctuating pressure signals show that this is a result of the formation of larger bubbles, when the fluidization regime is changed in the upper part of the bed. At the highest excess gas velocity the bubble flow becomes more constrained due to a more rapid coalescence of the bubbles and the tubes show Type A wastage profiles throughout the bed. (C) 2003 Elsevier Ltd. All rights reserved.
引用
收藏
页码:31 / 40
页数:10
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