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首页> 外文期刊>Journal of Fluid Mechanics >Stability of detonations for an idealized condensed-phase model
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Stability of detonations for an idealized condensed-phase model

机译:理想化凝聚相模型的爆轰稳定性

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The stability of travelling wave Chapman-Jouguet and moderately overdriven detonations of Zeldovich-von Neumann-Doring type is formulated for a general system that incorporates the idealized gas and condensed-phase (liquid or solid) detonation models. The general model consists of a two-component mixture with a one-step irreversible reaction between reactant and product. The reaction rate has both temperature and pressure sensitivities and has a variable reaction order. The idealized condensed-phase model assumes a pressure-sensitive reaction rate, a constant-gamma caloric equation of state for an ideal fluid, with the isentropic derivative gamma=3, and invokes the strong shock limit. A linear stability analysis of the steady, planar, ZND detonation wave for the general model is conducted using a normal-mode approach. An asymptotic analysis of the eigenmode structure at the end of the reaction zone is conducted, and spatial boundedness (closure) conditions formally derived, whose precise form depends on the magnitude of the detonation overdrive and reaction order. A scaling analysis of the transonic flow region for Chapman-Jouguet detonations is also studied to illustrate the validity of the linearization for Chapman-Jouguet detonations. Neutral stability boundaries are calculated for the idealized condensed-phase model for one- and two-dimensional perturbations. Comparisons of the growth rates and frequencies predicted by the normal-mode analysis for an unstable detonation are made with a numerical solution of the reactive Euler equations. The numerical calculations are conducted using a new, high-order algorithm that employs a shock-fitting strategy, an approach that has significant advantages over standard shock-capturing methods for calculating unstable detonations. For the idealized condensed-phase model, nonlinear numerical solutions are also obtained to study the long-time behaviour of one- and two-dimensional unstable Chapman-Jouguet ZND waves.
机译:对于包含理想化气体和冷凝相(液相或固相)爆轰模型的一般系统,制定了行波Chapman-Jouguet的稳定性和Zeldovich-von Neumann-Doring型的中度超速爆轰。通用模型由两组分混合物组成,反应物和产物之间具有一步不可逆的反应。反应速率同时具有温度和压力敏感性,并且具有可变的反应顺序。理想化的凝聚相模型假设压敏反应速率,理想流体的恒定伽马热力学状态方程(等熵导数伽马= 3)并引用强冲击极限。使用正常模式方法对常规模型的稳定,平面ZND爆震波进行了线性稳定性分析。在反应区末端对本征模结构进行渐近分析,并正式得出空间有界(封闭)条件,其精确形式取决于爆炸超速的幅度和反应顺序。还对查普曼-乔格顿爆轰的跨音速流动区域的比例分析进行了研究,以说明查普曼-乔格特爆轰线性化的有效性。计算一维和二维扰动的理想凝聚相模型的中性稳定边界。用反应性欧拉方程的数值解比较了由正常模式分析预测的不稳定爆轰的增长率和频率。数值计算是使用一种新的高阶算法进行的,该算法采用了减震拟合策略,该方法相对于用于计算不稳定爆震的标准减震方法具有明显优势。对于理想的凝聚相模型,还获得了非线性数值解,以研究一维和二维不稳定Chapman-Jouguet ZND波的长期行为。

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