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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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(a) Pseudo-Steady-State LLPTC model.The reaction relationship is given as1k app¼V K QX A þ V kQ ið31Þwhere denotes the reactivity <strong>of</strong> the phosphazene reaction. The plot <strong>of</strong> 1=k app versus , inwhich the data were measured at the initial time <strong>of</strong> different experimental runs, allows oneto obtain the mass transfer coefficient, K QX A, <strong>and</strong> the intrinsic reaction rate constant k,from the slope <strong>and</strong> intercept <strong>of</strong> the straight line.(b) Extrapolation Method. If mass transfer resistance influences the reaction, the concentration<strong>of</strong> the active catalyst QY cannot remain constant during the course <strong>of</strong> thereaction. Decreasing the concentration <strong>of</strong> organic reactant RX increases the apparentfirst-order reaction-rate constant. When the concentration <strong>of</strong> organic reactant decreases,both the reaction rate <strong>and</strong> the effect <strong>of</strong> mass transfer decrease. If the organic reactantconcentration extrapolates to zero ð½RXŠ !0Þ, the effect <strong>of</strong> mass transfer can beneglected. The intrinsic reaction-rate constant, k, is easily evaluated.(c) Half-Reaction in the Organic <strong>Phase</strong>. The organic reactant reacted with an intermediatecatalyst, tetra-n-butyl ammonium phenolate, in a homogeneous organic phase.The intrinsic reaction-rate constant was calculated from Eq. (12).Another LLPTC is usually performed in an agitated system, in which the organicphase is mostly dispersed. Several efforts have been made in developing the theory for atwo-liquid phase with chemical reactions. For an organic phase being the dispersed phase,several phenomena take place: (1) formation <strong>of</strong> a single droplet in the continuous phase bystirring, (2) free rise or fall <strong>of</strong> a droplet through the continuous phase, <strong>and</strong> (3) coalescence<strong>of</strong> a droplet at the end <strong>of</strong> the free-rise period. During the extraction <strong>of</strong> a catalytic intermediate,mass transfer from the bulk aqueous phase to the organic droplet surface influencesthe rate <strong>of</strong> PT reaction. Yang [71,72] studied the general analysis <strong>of</strong> the dynamics <strong>of</strong>a PT-catalytic reaction in a dispersed system <strong>of</strong> liquid–liquid phases, considering theirreversible <strong>and</strong> reversible reactions by solving the finite difference <strong>and</strong> Runge–Kuttafourth-order methods. The rates <strong>of</strong> change <strong>of</strong> RX, RY, QX, <strong>and</strong> QY in an organic dropletare described by the instantaneous equations <strong>of</strong> diffusion <strong>and</strong> reaction with the correspondinginitial <strong>and</strong> boundary conditions as follows:@ C i@t ¼ D i @r 2 @ C iþ @r @r iR; i ¼ RX; RY; QX; <strong>and</strong> QY ð32Þr 2where i is the stoichiometric coefficient <strong>of</strong> the i component.The kinetics <strong>of</strong> inverse PT-catalytic extraction <strong>of</strong> species into the water phase wascarried out with partially water-soluble pyridines or derivatives [36,38,40,59,73], as shownin mechanism (9). These reactions can be described by a pseudo-first-order hypothesis[38,40]:k app ¼ k h þ k c ½PNOŠ ið33ÞHowever, so far, the detailed kinetics <strong>of</strong> I-LLPTC are unclear.As mentioned above, the various approaches to LLPTC modeling have been taken,<strong>and</strong> a comprehensive general model for N-LLPTC reactions is widely held. However, akinetic model for I-LLPTC <strong>and</strong> R-LLPTC reactions is yet to be developed.Copyright © 2003 by Taylor & Francis Group, LLC

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