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11. Interfacial Mechanism and Kinetics of Phase-Transfer Catalysis

11. Interfacial Mechanism and Kinetics of Phase-Transfer Catalysis

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The extractive effectiveness factor , defined as the effect <strong>of</strong> the diffusion boundary layeron the extraction rate <strong>of</strong> quaternary salt can be characterized in terms <strong>of</strong> the ratio <strong>of</strong> Eq.(62) to Eq (65): ¼ K o m½QXŠ m½QXŠ k m m½QXŠ m½QXŠ ð66Þ¼ðBi o þ Bi a þ 1Þ 1in which Bi o ð¼ mk m =k o Þ <strong>and</strong> Bi a ð¼ mk m =k a Þ are Biot numbers for the organic phase <strong>and</strong>aqueous phase, respectively. Equation (66) represents the mass transfer ratio <strong>of</strong> conductionrate to convection rate <strong>of</strong> the quaternary salt at the interface. According to theexperimental data <strong>of</strong> Lin [127], the values <strong>of</strong> , Bi o ,<strong>and</strong>Bi a are calculated to be around0.96, 0.04, <strong>and</strong> 0.002, respectively, when the agitation rate is lower than 100 rpm. Hence, itclarified again that the membrane resistance at high agitation rates controls the masstransfer resistance <strong>of</strong> the membrane extraction.Usually, mass transfer coefficients can be correlated from the classical equation:Sh ¼ aRe b Sc cð67Þwhere Shð¼ k m d=DÞ is the Sherwood number; Re (¼ du=Þ is the Reynolds number, Sc(¼ =D) is the Schmidt number, D is the diffusivity in the bulk fluid, u is a characteristicvelocity <strong>of</strong> the fluid such as the mean fluid flow velocity, is the density, is the viscosity,<strong>and</strong> d is a characteristic dimension <strong>of</strong> the system.In Eq. (67), a is an experimental constant <strong>and</strong> c usually has a value <strong>of</strong> 1/3 [128–130].The value <strong>of</strong> b depends on the type <strong>of</strong> equipment <strong>and</strong> system, <strong>and</strong> most <strong>of</strong> the theoriespredict a one-half power on the Reynolds number [131]. The mass transfer from bulksolution to the surface <strong>of</strong> the membrane is mainly controlled by the turbulence <strong>of</strong> the fluidmotion created by stirring. The characteristic velocity is defined in terms <strong>of</strong> the stirringspeed ðu ¼ ndÞ. The values <strong>of</strong> a <strong>and</strong> b were determined from the intercept <strong>and</strong> slope <strong>of</strong> theline <strong>of</strong> Sh=Sc 1=3 against Re for the specified mass transfer coefficients <strong>of</strong> k a , k o , <strong>and</strong> K o .These parameters are different <strong>and</strong> are dependent on the system geometry <strong>and</strong> flow pattern.However, it can be concluded that the exponent value on Re varied from 0.2 to 1.0,depending on the design <strong>of</strong> the membrane permeation system.The correlating equation [67] established here can be used to evaluate the masstransfer coefficient <strong>and</strong> the thickness <strong>of</strong> the diffusion boundary layer, ð¼ d=shÞ. Thethickness <strong>of</strong> this layer calculated for an organic solvent <strong>and</strong> aqueous solution were10 3 –10 2 <strong>and</strong> 10 9 –10 7 cm, respectively, for the four types <strong>of</strong> quaternary salts studied.For a solute crossing a mass transfer resistance film, the transfer time can be approximatelyestimated by the following equation [131]:ðfilm thickness)2<strong>Transfer</strong> time ¼ð68Þdiffusion coefficientBased on the data presented here, the estimated transfer times for a solute crossing theorganic <strong>and</strong> aqueous mass transfer resistance film are about 1–10 <strong>and</strong> 10 11 –10 8 s, respectively.E. <strong>Interfacial</strong> Phenomena in LLPTCStarks [132] proposed that the transfer rate <strong>of</strong> an anion across the interface is largelygoverned by four factors: (1) interfacial area, (2) anion activity <strong>and</strong> hydration at theCopyright © 2003 by Taylor & Francis Group, LLC

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