首页> 外文会议>International Mechanical Engineering Congress and Exposition >(V08CT09A040)EQUATION TWO-FLUID MODEL ANALYSIS FOR STRATIFIED FLOW UNDER KINEMATIC AND DYNAMIC INSTABILITIES
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(V08CT09A040)EQUATION TWO-FLUID MODEL ANALYSIS FOR STRATIFIED FLOW UNDER KINEMATIC AND DYNAMIC INSTABILITIES

机译:(V08CT09A040)在运动型和动态稳定性下分层流动的方程式两种流体模型分析

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The unstable one-dimensional incompressible two-fluid model including a hydrostatic force is reduced to a two equation model in terms of the liquid volume fraction and the liquid velocity. For small density ratios the model may be simplified to a formulation that is equivalent tothe Shallow Water Theory (SWT) equations [Whitham, 1975] with a source term corresponding to the two-fluid model constitutive relations for wall and interfacial shear and to a void gradient term that contains the Kelvin-Helmholtz mechanism. Linear stability of the SWT equations shows that the model is made well-posed stable by the hydrostatic force. However, unlike the SWT equations, the two equation two-fluid model is only conditionally stable. As the gas velocity increases the model becomes unstable once the kinematic instability occurs, i.e., the Viscous Kelvin-Helmholtz (VKH) instability. When the gas velocity is increased further the model becomes dynamically unstable, i.e., it reaches the InviscidKelvin-Helmholtz (IKH) instability limit. Beyond the IKH limit the model becomes ill-posed and requires higher order modelling, e.g. surface tension. Simple analytic expressions for the two instabilities are obtained because of the simplified mathematics of the two equation model. Furthermore, the wave "sheltering" effect, which allows more accurate predictions of the flow regime transition, may be easily incorporated into the analysis. The theory is validated with the new HAWAC flow regime map [Vallee et al., 2010].
机译:在液体体积分数和液体速度方面,包括静压力的不稳定的一维不可压缩的双流体模型包括静水力和两个方程模型。对于小密度比率,模型可以简化到等同于浅水理论(SWT)方程的制剂[Whitham,1975],其源期对应于壁和界面剪切的双流体模型构成关系以及空隙包含Kelvin-Helmholtz机制的梯度术语。 SWT方程的线性稳定性表明,该模型由静水力稳定地稳定。然而,与SWT方程不同,两个方程两种流体模型仅有条件稳定。由于气体速度增加,一旦运动不稳定性发生,即,就能变得不稳定,即粘性Kelvin-Helmholtz(VKH)不稳定性。当进一步增加气体速度时,模型变得动态不稳定,即,它到达Inciscidkelvin-Helmholtz(IKH)不稳定限制。除了IKH限制之外,模型变得不良,需要更高阶建模,例如更高阶建模。表面张力。由于两个等式模型的简化数学,获得了两个不稳定性的简单分析表达式。此外,可以容易地结合到分析中的允许更准确地预测流动调节的波“避难”效应。该理论用新的Hawac Flow Endime Map [Vallee等,2010]。

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