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Interpretation of gas residence time distributions in large airlift tower loop reactors
Authors:H M Rüffer  Liwei Wan  A Lübbert  K Schügerl
Institution:(1) Institut für Technische Chemie, Universität Hannover, Callinstr. 3, D-30167 Hannover, Germany;(2) Present address: Hoechst Co, Höchst
Abstract:Gas-residence time distribution (RTD) response curves measured in a 23 m high pilot plant airlift tower loop reactor, which consisted of a riser, a special downcomer construction and at the top of the riser a large head. The measurements were evaluated by means of a deterministic dispersion model, which yielded the following particular parameters for the riser, downcomer and the head: Gas-Bo numbers, gas-mean residence times, gas holdups, liquid velocities, gas and liquid circulation times as well as a fraction of the large and small bubbles in a model medium (water) and during cultivation of baker's yeast.List of Symbols A cross section - Bo Bodenstein number - Bo d (= l d w G,d /D d ) - Bo h (= l h w G,h /D h ) - Bo r (= l r w G,r /D r ) - D longitudinal dispersion coefficient - E gas holdup - E(t) RTD-density function - L, l length parameter - q fraction of the gas throughput which is not recirculated (approximately equal to fraction of the large bubbles) - r fraction of the throughput which is recirculated (approximately equal to the fraction of the small bubbles) - t c circulation time - t cL liquid circulation time - t c,L * liquid circulation time calculated from the measured w Ld in the downcomer - V h hydrodynamical calculated gas-liquid volume - V d h (=V d+0.75/2 V k ) - V k h =(0.25V k ) - V r h = (V r+0.75/2 V k ) - V L liquid volume - V G dispersed gas volume - V G * gas throughput at the gas distributor (given in m3/h) under standard conditions, 1 bar and 25°C) - V G,d * gas throughput in downcomer (=V G * agr) - V G,h * gas throughput in head (=V G * ) - V G,r * gas throughput in riser (V G * (1+agr) - w g gas velocity - w G,rel relative gas velocity with respect to the liquid velocity w L - w G,d gas velocity in the downcomer (=w G,rel –w Ld ) - w G,h gas velocity in the head (=w G,rel ) (since wLh = o) - w G,r gas velocity in the riser (=w G,rel +w Lr ) - w L liquid velocity - w L,d liquid velocity in the downcomer measured with mass flow meter - w sg ·w SL superficial gas and liquid velocities - mgr first moment of the response curve - tau mean residence time Indices d downcomer - G gas phase - h head - L liquid phase - r riser - h hydrodynamic (upper position) Dedicated to the 65th birthday of Proffessor Fritz Wagner.The authors gratefully acknowledge the financial support by the Krupp Industrietechnik, Grevenbroich and the support of Pleser Co, Darmstadt. H. M. Rüffer thanks the Verband der Chemischen Industrie for a Fond der Chemie scholarship, and W. Liwei thanks the government of Lower Saxony for a graduate scholarship.
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