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Boreskov Institute of Catalysis of the Siberian Branch of Russian ...

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PP-I-2LATERAL INTERACTIONS, FINITE MOBILITY ANDMULTIPLICITY OF STEADY STATES FOR LANGMUIR –HINSHELWOOD MECHANISM. MONTE CARLO ANDTRANSFER-MATRIX TECHNIQUESJu.A. Brizhanskaja*, L.V. Brizhanskii*, A.V. Myshlyavtsev* , **, M.D. Myshlyavtseva**Omsk State Technical University, Omsk, Russia**<strong>Institute</strong> <strong>of</strong> Hydrocarbons Processing SB RAS, Omsk, RussiaThe simplest model for CO oxidation on platinum surface is <strong>the</strong> well known three stepsLangmuir-Hinshelwood mechanismA 2+ 2Z ↔ 2AZ; B + Z ↔ BZ; AZ + BZ → AB + 2Z,(1)where AZ and BZ are <strong>the</strong> adsorbed species on <strong>the</strong> catalyst Z, and A 2 , B and AB <strong>the</strong> gas phasesubstances. The conventional mean-field (MF) kinetic equations can be written as [1]A( 1−x − y)( 1−x − y)−22⎪⎧dx / dt = 2k1P− 2k−x − k xy2 1 3⎨, (2)⎪⎩ dy / dt = k2PBk−2y − k3xywhere x and y are <strong>the</strong> adsorbate coverages, P and <strong>the</strong> reactant pressures, and k , k 1,k , −1 k−2 3, k <strong>the</strong> rate constants for adsorption, desorption and reaction, respectively; t is time.For simplicity we are going to consider <strong>the</strong> case <strong>of</strong> irreversible adsorption (= 0). Forsome parameter sets <strong>the</strong>re exists <strong>the</strong> domain <strong>of</strong> <strong>the</strong> multiplicity <strong>of</strong> <strong>the</strong> steady states in <strong>the</strong>plane( lg P , lg P )2ABA 2PB2k , − 1k−2. This domain contains only two internal steady states. The simplest MFequations (2) ignore <strong>the</strong> non-ideality <strong>of</strong> surface rate processes. We considered earlier <strong>the</strong> MFequations incorporating <strong>the</strong> adsorbate-adsorbate lateral interactions via <strong>the</strong> coveragedependence <strong>of</strong> <strong>the</strong> rate constants. It is known that in <strong>the</strong> frameworks <strong>of</strong> <strong>the</strong> lattice gas modeland <strong>the</strong> transition state <strong>the</strong>ory <strong>the</strong>re are <strong>the</strong> exact expressions for <strong>the</strong> rate constants. Weconsidered a lattice gas model as a model <strong>of</strong> adsorbed overlayer. Two kind <strong>of</strong> adsorbedspecies can occupy lattice sites <strong>of</strong> a square lattice. We take into account only nearest-neighborlateral interactions. Within <strong>the</strong> framework <strong>of</strong> our model <strong>the</strong> exact analytical expressions <strong>of</strong> <strong>the</strong>right hand parts <strong>of</strong> equations (1) are absent and hence we should use an approximatetechnique. It is well known, that <strong>the</strong> one <strong>of</strong> <strong>the</strong> most effective approach is <strong>the</strong> transfer matrixmethod. Using <strong>the</strong> latter approach one can solve <strong>the</strong> problem <strong>of</strong> deriving expressions for <strong>the</strong>rate constants as functions <strong>of</strong> concentration. Experience shows that <strong>the</strong> transfer matrixtechnique yields very good results. It was shown that <strong>the</strong> number <strong>of</strong> <strong>the</strong> internal steady statescan be equal to arbitrary integer number. We have studied numerically twenty seven models214

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