首页> 外文会议>American Society of Mechanical Engineers(ASME) Joint U.S.-European Fluids Engineering Division Summer Conference 2006(FEDSM2006) vol.1 pt.A; 20060717-20; Miami,FL(US) >NUMERICAL SIMULATIONS OF UNSTEADY WET STEAM FLOWS WITH NON-EQUILIBRIUM CONDENSATION IN THE NOZZLE AND THE STEAM TURBINE
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NUMERICAL SIMULATIONS OF UNSTEADY WET STEAM FLOWS WITH NON-EQUILIBRIUM CONDENSATION IN THE NOZZLE AND THE STEAM TURBINE

机译:喷嘴和汽轮机中非平衡凝结的非稳态湿蒸汽流的数值模拟

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Numerical techniques for non-equilibrium condensing flows are presented. Conservation equations for homogeneous gas-liquid two-phase compressible flows are solved by using a finite volume method based on an approximate Riemann solver. The phase change consists of the homogeneous nucleation and growth of existing droplets. Nucleation is computed with the classical Volmer-Frenkel model, corrected for the influence of the droplet temperature being higher than the steam temperature due to latent heat release. For droplet growth, two types of heat transfer model between droplets and the surrounding steam are used: a free molecular flow model and a semi-empirical two-layer model which is deemed to be valid over a wide range of Knudsen number.rnThe computed pressure distribution and Sauter mean droplet diameters in a convergent-divergent (Laval) nozzle are compared with experimental data. Both droplet growth models capture qualitatively the pressure increases due to sudden heat release by the non-equilibrium condensation. However the agreement between computed and experimental pressure distributions is better for the two-layer model. The droplet diameter calculated by this model also agrees well with the experimental value, whereas that predicted by the free molecular model is too small.rnCondensing flows in a steam turbine cascade are calculated at different Mach numbers and inlet superheat conditions and are compared with experiments. Static pressure traverses downstream from the blade and pressure distributions on the blade surface agree well with experimental results in all cases. Once again, droplet diameters computed with the two-layer model give best agreement with the experiments. Droplet sizes are found to vary across the blade pitch due to the significant variation in expansion rate. Flow patterns including oblique shock waves and condensation-induced pressure increases arernalso presented and are similar to those shown in the experimental Schlieren photographs.rnFinally, calculations are presented for periodically unsteady condensing flows in a low expansion rate, convergent-divergent (Laval) nozzle. Depending on the inlet stagnation subcooling, two types of self-excited oscillations appear: a symmetric mode at lower inlet subcooling and an asymmetric mode at higher subcooling. Plots of oscillation frequency versus inlet sub-cooling exhibit a hysteresis loop, in accord with observations made by other researchers for moist air flow.
机译:提出了非平衡冷凝流的数值技术。利用基于近似黎曼(Riemann)求解器的有限体积方法,求解了均相气液两相可压缩流的守恒方程。相变包括现有液滴的均匀成核和生长。用经典的Volmer-Frenkel模型计算成核作用,并校正了由于潜热释放而导致的液滴温度高于蒸汽温度的影响。对于液滴的生长,使用了两种类型的液滴与周围蒸汽之间的传热模型:一个自由分子流动模型和一个半经验两层模型,这些模型在广泛的克努森数范围内被认为是有效的。将收缩-发散(拉伐)喷嘴中的分布和Sauter平均液滴直径与实验数据进行比较。两种液滴生长模型定性地捕获了由于非平衡冷凝突然释放的热量而导致的压力增加。但是,对于两层模型,计算压力分布和实验压力分布之间的一致性更好。该模型计算出的液滴直径也与实验值吻合,而自由分子模型预测的液滴直径太小。在不同的马赫数和入口过热条件下,计算了汽轮机叶栅中的冷凝流,并与实验进行了比较。在所有情况下,静压都在叶片的下游移动,叶片表面的压力分布与实验结果非常吻合。再次,用两层模型计算的液滴直径与实验最吻合。由于膨胀率的显着变化,发现液滴的大小在整个叶片螺距上都会变化。还介绍了包括斜向冲击波和凝结引起的压力增加的流态,并且与实验Schlieren照片中显示的流态相似。最后,给出了针对低膨胀率,会聚-发散(拉瓦尔)喷嘴中的周期性非稳态凝结流的计算。取决于入口停滞过冷,会出现两种类型的自激振荡:较低入口过冷的对称模式和较高过冷的不对称模式。振荡频率与入口过冷的关系图显示出一个磁滞回线,这与其他研究人员对潮湿空气流动的观察结果一致。

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