针对超声速气流驱动干粉颗粒形成的缩放喷管气固两相射流,采用拉格朗日方法、气固双向耦合模型以及Shear-Stress Transport k-ω湍流模型进行数值模拟,分析了颗粒装载比、萨夫曼力和入口压力等因素对气体参数、颗粒速度以及颗粒聚集度...针对超声速气流驱动干粉颗粒形成的缩放喷管气固两相射流,采用拉格朗日方法、气固双向耦合模型以及Shear-Stress Transport k-ω湍流模型进行数值模拟,分析了颗粒装载比、萨夫曼力和入口压力等因素对气体参数、颗粒速度以及颗粒聚集度的影响。结果表明:气固双向耦合模型可以准确的分析气体与颗粒之间的相互作用。当高压气体通过缩放喷管时会产生超声速流动,从而带动颗粒作加速运动;在同一入口压力下,如果颗粒装载比较高,那么颗粒速度较小,且气体参数受颗粒的影响较大。颗粒在喷管扩张段轴线附近聚集,导致轴线到壁面附近区域内,产生沿径向向外的气流速度梯度,这可以解释萨夫曼力使轴线上气固两相的速度增大,并且在高颗粒装载比下的影响更显著的原因。不同入口压力下可能出现欠膨胀、过膨胀和完全膨胀三种不同喷管射流形态;在完全膨胀流态下,颗粒加速和气流降温的效果相对更好。研究结果可为超声速干粉灭火技术的应用提供理论支撑。展开更多
Particle coagulation by Brownian motion is an important but difficult research topic.When particle volume concentration is larger than 0.1%,the classic SMOLUCHOWSKI equation is not applicative anymore.The high concent...Particle coagulation by Brownian motion is an important but difficult research topic.When particle volume concentration is larger than 0.1%,the classic SMOLUCHOWSKI equation is not applicative anymore.The high concentration coagulation,with HEINE's correction,source terms for the Taylor-series expansion method of moments(TEMOM) are firstly driven in this paper.Ultra-fine particle(d0?100 mm) with initial volume fraction f?1% coagulation in a planar jet turbulence flow is simulated via the large eddy simulation(LES).The instantaneous and time-averaged particle distributions and the high concentration enhancement are given out.The particle number concentration distribution results show that the coagulation is more intense comparing to dilute case in previous research,especially near the nozzle exit.After jet flow is fully developed,the effect is much more obvious at the region between vortexes.The time-averaged γ(the high concentration enhance factor) distributes sharply and symmetrically about the jet centerline at the upstream,but becomes broad and flat at downstream where the cross-stream averaged γ fluctuates drastically.As a new attempt,this paper shows Brownian coagulation with high concentration also can be calculated via TEMOM appropriately,and the coagulation at the region between vortexes is about 1.38 times intensive of the dilute result calculated by the classic Smoluchowski theory.展开更多
文摘针对超声速气流驱动干粉颗粒形成的缩放喷管气固两相射流,采用拉格朗日方法、气固双向耦合模型以及Shear-Stress Transport k-ω湍流模型进行数值模拟,分析了颗粒装载比、萨夫曼力和入口压力等因素对气体参数、颗粒速度以及颗粒聚集度的影响。结果表明:气固双向耦合模型可以准确的分析气体与颗粒之间的相互作用。当高压气体通过缩放喷管时会产生超声速流动,从而带动颗粒作加速运动;在同一入口压力下,如果颗粒装载比较高,那么颗粒速度较小,且气体参数受颗粒的影响较大。颗粒在喷管扩张段轴线附近聚集,导致轴线到壁面附近区域内,产生沿径向向外的气流速度梯度,这可以解释萨夫曼力使轴线上气固两相的速度增大,并且在高颗粒装载比下的影响更显著的原因。不同入口压力下可能出现欠膨胀、过膨胀和完全膨胀三种不同喷管射流形态;在完全膨胀流态下,颗粒加速和气流降温的效果相对更好。研究结果可为超声速干粉灭火技术的应用提供理论支撑。
基金supported by National Natural Science Foundation of China (Grant No. 50976107)National Key Technology R&D Program of China (Grant No. 2009BAF39B01)the Science Foundation of Zhejiang Sci-Tech University (ZSTU) of China (Grant No. 1003808-Y)
文摘Particle coagulation by Brownian motion is an important but difficult research topic.When particle volume concentration is larger than 0.1%,the classic SMOLUCHOWSKI equation is not applicative anymore.The high concentration coagulation,with HEINE's correction,source terms for the Taylor-series expansion method of moments(TEMOM) are firstly driven in this paper.Ultra-fine particle(d0?100 mm) with initial volume fraction f?1% coagulation in a planar jet turbulence flow is simulated via the large eddy simulation(LES).The instantaneous and time-averaged particle distributions and the high concentration enhancement are given out.The particle number concentration distribution results show that the coagulation is more intense comparing to dilute case in previous research,especially near the nozzle exit.After jet flow is fully developed,the effect is much more obvious at the region between vortexes.The time-averaged γ(the high concentration enhance factor) distributes sharply and symmetrically about the jet centerline at the upstream,but becomes broad and flat at downstream where the cross-stream averaged γ fluctuates drastically.As a new attempt,this paper shows Brownian coagulation with high concentration also can be calculated via TEMOM appropriately,and the coagulation at the region between vortexes is about 1.38 times intensive of the dilute result calculated by the classic Smoluchowski theory.