Abstract

An experiment was carried out for investigating pressure behavior of catalyst powders, with a Sauter mean diameter of 63.6 μm, flowing downward in a cyclone dipleg with 150 mm inner diameter and 9000 mm high. Time mean pressure and time series of pressure fluctuations were measured at different axial positions in the dipleg with particle mass fluxes ranging from 50.0 to 385.0 kg m−2 s−1. The experimental results showed that the time mean pressure in the dipleg increased progressively from the top section to the bottom section. The experimental phenomena displayed that the fluidization patterns in the dipleg can be divided into two types on the whole, namely the dilute–dense coexisting falling flow and the dense conveying flow along the dipleg. In the dilute–dense coexisting falling flow, the dilute phase region was composed of a length of swirling flow below the inlet of dipleg and a dilute falling flow above the dense bed level. With increasing particle mass flux, the dilute–dense coexisting falling flow was gradually transformed to be the dense conveying flow, and the exit pressure of the dipleg increased considerably. The pressure fluctuations were closely related to the fluidization patterns inside the dipleg. In the dilute–dense coexisting falling flow, the pressure fluctuations in the dilute flow region originated from particle clusters, propagating downward as a pressure wave; however, the pressure fluctuations in the dense flow region originated from rising gas bubbles, propagating upward. When the dense conveying flow was formed in the dipleg, the pressure fluctuations originated mainly from instability of the feed and the compressed gas, propagating downward. The standard deviation of the pressure fluctuations indicated that the intensity of pressure fluctuations first increased and then decreased with increasing particle flux.

Highlights

  • Edited by Xiu-Qin ZhuIn gas–solid circulating fluidized (CFB) beds, the particles are collected by cyclones and returned into a fluidized bed along a cyclone dipleg conveying system

  • The former was caused by the falling particle clusters interacting with the up flowing gas, and the latter was caused by the bubbles rising in the dense flow

  • This paper presents an experimental study on the pressure behaviors of a catalyst powder flowing down in a dipleg with 150 mm i.d. and 9000 mm high

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Summary

Introduction

In gas–solid circulating fluidized (CFB) beds, the particles are collected by cyclones and returned into a fluidized bed along a cyclone dipleg (dip-leg) conveying system. One of the flow characteristics in the dipleg is that the particle velocity is greater than gas velocity, so the direction of slip velocity between gas and particles is upward Another one is the particle flow is usually against a negative pressure gradient. These two characteristics lead to the complexity of fluidization pattern and flow instability in the dipleg, which demonstrates that there are more than one different fluidization pattern coexisting and distinctive pressure fluctuations in the dipleg (Kunni and Levenspiel 1991; Hoffmann and Stein 2002; Cortes and Gil 2007). Little work has been done on gas-particle flow instability involving the cyclone dipleg; the relationship between the pressure fluctuations and the fluidization regime transitions, and the effect particle mass flux on the pressure fluctuations, is rarely reported.

Experimental
Flow phenomena in the dipleg
Time mean pressure profiles in the dipleg
Pressure fluctuation
Standard deviation of the pressure fluctuations
Conclusions
Full Text
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