首页> 外文期刊>Chemical Engineering Research & Design: Transactions of the Institution of Chemical Engineers >Influence of liquid viscosity and surface tension on the gas-liquid mass transfer coefficient for solid foam packings in co-current two-phase flow
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Influence of liquid viscosity and surface tension on the gas-liquid mass transfer coefficient for solid foam packings in co-current two-phase flow

机译:并流两相流中液体粘度和表面张力对固体泡沫填料气-气传质系数的影响

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摘要

The gas-liquid mass transfer coefficient and other hydrodynamic parameters such as liquid holdup and frictional pressure drop are presented for gas and liquid moving in co-current upflow and downfiow through solid foam packings of 10 and of 40 pores per linear inch(ppi).The effect of increasing the liquid viscosity on the mass transfer coefficient in co-current upflow is quantified and correlated to the frictional pressure drop,a measure of the frictional energy dissipation:k_La_(GL)epsilon_L(Sc_L/Sc_(water))~(0.69)=2.05 X 10~(-4)P_f~(0.8)(m_L~3 m_p~(-3)s~(-1)).The gas-liquid mass transfer coefficient in co-current downfiow is correlated to the liquid velocity and the Schmidt number using the correlation proposed by Sherwood and Holloway[Sherwood,T.and Holloway,E,1940,Performance of packed towers-liquid film data for several packings,Transactions of the American Institute of Chemical Engineers 36:39-70]:k_L a_(GL)epsilon_L D_L~(-1)=3.7(u_(L rho L mu_L)~(-1))~(1.16)(Sc_L)~(0.5)(m_L m_p~(-3)).The results for the gas-liquid mass transfer coefficient in co-current upflow were correlated with a similar equation,where the influence of the gas velocity is included,similar to the correlations for packed beds of spherical particles proposed in Fukushima and Kusaka[Fukushima,S.and Kusaka,K.,1979,Gas-liquid mass transfer and hydrodynamic flow region in packed columns with cocurrent upward flow,Journal of Chemical Engineering of Japan 12(4):296-301]:k_L a_(GL)epsilon_L D_L~(-1)=311u_G~(0.44)(u_(L rho L mu_L~(-1))~(0.92)(Sc_L)~(0.5)(m_L m_p~(-3)).In this study the liquid Schmidt number dependency of the gas-liquid mass transfer coefficient points to the penetration theory describing the rate of mass transfer for gas-liquid flow through solid foam packings.
机译:给出了气/液传质系数和其他流体力学参数,例如液体滞留率和摩擦压降,这些气体和液体通过每线性英寸(ppi)10和40个孔的固体泡沫填料并流向上和向下流动。量化并发流动中增加液体粘度对传质系数的影响,并将其与摩擦压降相关联,该摩擦压降是摩擦能量耗散的量度:k_La_(GL)epsilon_L(ScL / Sc_(水))〜( 0.69)= 2.05 X 10〜(-4)P_f〜(0.8)(m_L〜3 m_p〜(-3)s〜(-1))。顺流向下的气液传质系数与利用Sherwood和Holloway提出的相关性[Sherwood,T。and Holloway,E,1940,填充塔的性能-几种填料的液膜数据],液体速度和Schmidt数,美国化学工程师学会学报36:39- 70]:k_L a_(GL)epsilon_L D_L〜(-1)= 3.7(u_(L rho L mu_L)〜(-1))〜(1.16)(Sc_L)〜(0.5)(m_L m_p〜 (-3))。并流上流中气液传质系数的结果与一个类似的方程式相关,其中包括了气体速度的影响,类似于在本文中提出的球形颗粒填充床的相关性Fukushima and Kusaka [Fukushima,S. and Kusaka,K.,1979,并流向上流动的填充塔中的气液传质和流体动力流动区域,日本化学工程学报12(4):296-301]:k_L a_(GL)epsilon_L D_L〜(-1)= 311u_G〜(0.44)(u_(L rho L mu_L〜(-1))〜(0.92)(Sc_L)〜(0.5)(m_L m_p〜(-3))在这项研究中,气液传质系数对液体施密特数的依赖性指向渗透理论,该理论描述了气液流经固体泡沫填料的传质速率。

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