A numerical scheme describing the oxidation process induced by single and multiple dielectric barrier discharges in a H 2 /O 2 /Ar mixture is developed. Path flux and sensitivity analyses are performed in order to identify important reaction paths. The analyses are conducted for an initial mixture of 2000 ppm H 2 and 3000 ppm O 2 balanced in Ar at a constant pressure of 1 atm and temperatures ranging from 474 K to 1008 K, covering both below and above the second explosion limit. Results with only one discharge as well as with repetitive discharges at rates between 1 kHz and 5 kHz are discussed. Three sets of reaction schemes leading to H 2 O formation are identified: two short-time-scale schemes involving negative ions and O( 1 D), respectively, and a long-timescale scheme involving ground state radicals, which is responsible for the majority of the H 2 O formation and driven by plasma dissociation of H 2 and O 2 . At temperatures below the second explosion limit, the last scheme drives the straight chain propagation mechanism without causing exponential growth of radicals, where the reactions of HO 2 play important roles on the overall fuel oxidation. At temperatures above the second explosion limit, H and O atoms produced from the dissociation of reactants by deactivation of excited argon subsequently trigger ignition significantly reducing the ignition delay. The consumption of H 2 and O 2 which follows is governed by conventional high temperature chain branching kinetics and occurs at a rate equivalent to that of the purely thermal reaction. Increasing the pulse repetition rate of the discharge at low temperatures results in a shift of the rate-limiting steps from reactions of H atoms to those of the OH radical. Furthermore, the kinetics of metastable Ar *m , HO 2 , O 2 (a 1 Δ g ), and O( 1 D) are analyzed and their implications to other systems are discussed. counterparts [5] due to their high energy. The kinetics governing PAC can be conceptually summarized into a three step process: (1) the creation of high-energy species by electron-impact processes, (2) reactions of the high-energy species with other species, and (3) their subsequent influences on the overall oxidation mechanism. The electron-impact processes themselves are relatively well understood, especially for common gases such as Ar, N 2 , O 2 , or H 2 . For modeling purposes, databases of electron impact collision cross sections for a desired gas are readily available [6]. Using a Boltzmann equation solver (e.g., BOLSIG+ [7]), the electron energy distribution function (EEDF) can be obtained for a given temperature, mixture, and E/N. From the EEDF, the production rates of high-energy species can be determined. Such high-energy species may be roughly divided into four types: ground state radicals, electronically excited species, ions, and vibrationally excited species. The ground state radicals, which include reactant fragments such as O or H atoms, are already incorporated in conventional combustion reaction mechanisms. Thus, their roles in fuel o...