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Influence of gas distribution and regime transitions on liquid velocity and turbulence in a 3-D bubble column

Identifieur interne : 000977 ( Istex/Corpus ); précédent : 000976; suivant : 000978

Influence of gas distribution and regime transitions on liquid velocity and turbulence in a 3-D bubble column

Auteurs : Ch Vial ; R. Lainé ; S. Poncin ; N. Midoux ; G. Wild

Source :

RBID : ISTEX:275345C20CC9F759B76EC486319A7E5A5E479C17

English descriptors

Abstract

Abstract: Laser Doppler anemometry has been applied to a bubble column equipped successively with three different gas distributors: a single-orifice nozzle, a multiple-orifice sparger and a porous plate. Axial and tangential mean and rms liquid velocity values have been measured up to a gas hold-up of 15–20%. A simple analytical model based on a bubble-induced turbulence is shown to be consistent with the results obtained with the three spargers and is used to estimate the Reynolds shear stress. The evolution of the local hydrodynamic parameters of the liquid phase with UG is explained and related to the hydrodynamic regime, the uniformity of the gas distribution and the start-up procedure.

Url:
DOI: 10.1016/S0009-2509(00)00325-0

Links to Exploration step

ISTEX:275345C20CC9F759B76EC486319A7E5A5E479C17

Le document en format XML

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<div type="abstract" xml:lang="en">Abstract: Laser Doppler anemometry has been applied to a bubble column equipped successively with three different gas distributors: a single-orifice nozzle, a multiple-orifice sparger and a porous plate. Axial and tangential mean and rms liquid velocity values have been measured up to a gas hold-up of 15–20%. A simple analytical model based on a bubble-induced turbulence is shown to be consistent with the results obtained with the three spargers and is used to estimate the Reynolds shear stress. The evolution of the local hydrodynamic parameters of the liquid phase with UG is explained and related to the hydrodynamic regime, the uniformity of the gas distribution and the start-up procedure.</div>
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<note type="content">Fig. 1: Different types of gas sparger used.</note>
<note type="content">Fig. 2: LDA data rates at different gas flow rates and radial positions with and without seeding.</note>
<note type="content">Fig. 3: Influence of gas distributor and gas flow rate on flow pattern (Hom.=HomogeneousHet.=Heterogeneous).</note>
<note type="content">Fig. 4: Evolution of the optimised values of the exponent m (Eq. 1).</note>
<note type="content">Fig. 5: Radial evolution of the mean axial liquid velocity component with UG.</note>
<note type="content">Fig. 6: Radial evolution of the rms liquid with UG.</note>
<note type="content">Fig. 7: Evolution of the liquid centreline velocity vC with UG for the three spargers.</note>
<note type="content">Fig. 8: Evolution of the centreline turbulence intensity IC with UG for the three spargers.</note>
<note type="content">Fig. 9: Radial evolution of the rms liquid with UG using the multiple-orifice distributor.</note>
<note type="content">Fig. 10: Theoretical velocity profile in a bubble column.</note>
<note type="content">Fig. 11: Comparison of experiments and theoretical velocity profiles.</note>
<note type="content">Fig. 12: Evolution of the optimized averaged mixing length 〈lm〉 with UG and the three spargers.</note>
<note type="content">Fig. 13: Evolution of τw with UG for the three spargers.</note>
<note type="content">Fig. 14: Radial evolution of the Reynolds shear stress with UG for the columns equipped with the porous plate.</note>
<note type="content">Fig. 15: Evolution of τw with UG for the three spargers.</note>
<note type="content">Table 1: Turbulence models compared in this work</note>
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<ce:simple-para view="all" id="simple-para.0090">Laser Doppler anemometry has been applied to a bubble column equipped successively with three different gas distributors: a single-orifice nozzle, a multiple-orifice sparger and a porous plate. Axial and tangential mean and rms liquid velocity values have been measured up to a gas hold-up of 15–20%. A simple analytical model based on a bubble-induced turbulence is shown to be consistent with the results obtained with the three spargers and is used to estimate the Reynolds shear stress. The evolution of the local hydrodynamic parameters of the liquid phase with
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<abstract lang="en">Abstract: Laser Doppler anemometry has been applied to a bubble column equipped successively with three different gas distributors: a single-orifice nozzle, a multiple-orifice sparger and a porous plate. Axial and tangential mean and rms liquid velocity values have been measured up to a gas hold-up of 15–20%. A simple analytical model based on a bubble-induced turbulence is shown to be consistent with the results obtained with the three spargers and is used to estimate the Reynolds shear stress. The evolution of the local hydrodynamic parameters of the liquid phase with UG is explained and related to the hydrodynamic regime, the uniformity of the gas distribution and the start-up procedure.</abstract>
<note type="content">Fig. 1: Different types of gas sparger used.</note>
<note type="content">Fig. 2: LDA data rates at different gas flow rates and radial positions with and without seeding.</note>
<note type="content">Fig. 3: Influence of gas distributor and gas flow rate on flow pattern (Hom.=HomogeneousHet.=Heterogeneous).</note>
<note type="content">Fig. 4: Evolution of the optimised values of the exponent m (Eq. 1).</note>
<note type="content">Fig. 5: Radial evolution of the mean axial liquid velocity component with UG.</note>
<note type="content">Fig. 6: Radial evolution of the rms liquid with UG.</note>
<note type="content">Fig. 7: Evolution of the liquid centreline velocity vC with UG for the three spargers.</note>
<note type="content">Fig. 8: Evolution of the centreline turbulence intensity IC with UG for the three spargers.</note>
<note type="content">Fig. 9: Radial evolution of the rms liquid with UG using the multiple-orifice distributor.</note>
<note type="content">Fig. 10: Theoretical velocity profile in a bubble column.</note>
<note type="content">Fig. 11: Comparison of experiments and theoretical velocity profiles.</note>
<note type="content">Fig. 12: Evolution of the optimized averaged mixing length 〈lm〉 with UG and the three spargers.</note>
<note type="content">Fig. 13: Evolution of τw with UG for the three spargers.</note>
<note type="content">Fig. 14: Radial evolution of the Reynolds shear stress with UG for the columns equipped with the porous plate.</note>
<note type="content">Fig. 15: Evolution of τw with UG for the three spargers.</note>
<note type="content">Table 1: Turbulence models compared in this work</note>
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<topic>Bubble column</topic>
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