Interfacial Reaction Kinetics

نویسندگان

  • BEN O’SHAUGHNESSY
  • DIMITRIOS VAVYLONIS
چکیده

We study A-B reaction kinetics at a fixed interface separating two immiscible bulk phases, A and B. Coupled equations are derived for the hierarchy of many-body correlation functions. Postulating physically motivated bounds, closed equations result without the need for ad hoc decoupling approximations. We consider general dynamical exponent z, where xt ∼ t is the rms diffusion distance after time t. At short times the number of reactions per unit area, Rt, is 2nd order in the far-field reactant densities n ∞ A , n ∞ B . For spatial dimensions d above a critical value dc = z − 1, simple mean field (MF) kinetics pertain, Rt ∼ Qbtn∞A n∞B where Qb is the local reactivity. For low dimensions d < dc, this MF regime is followed by 2nd order diffusion controlled (DC) kinetics, Rt ≈ x t n∞A n∞B , provided Qb > Q∗b ∼ (n∞B ). Logarithmic corrections arise in marginal cases. At long times, a cross-over to 1st order DC kinetics occurs: Rt ≈ xtn∞A . A density depletion hole grows on the more dilute A side. In the symmetric case (n∞A = n ∞ B ), when d < dc the long time decay of the interfacial reactant density, nA, is determined by fluctuations in the initial reactant distribution, giving n s A ∼ t. Correspondingly, A-rich and B-rich regions develop at the interface analogously to the segregation effects established by other authors for the bulk reaction A + B → ∅. For d > dc fluctuations are unimportant: local mean field theory applies at the interface (joint density distribution approximating the product of A and B densities) and nA ∼ t. We apply our results to simple molecules (Fickian diffusion, z = 2) and to several models of short-time polymer diffusion (z > 2). PACS numbers: 05.40.+j, 68.45.Da, 82.35.+t

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تاریخ انتشار 1998