共查询到19条相似文献,搜索用时 78 毫秒
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限流沿对撞壁射流近壁区混合过程影响的实验研究(二) 总被引:3,自引:0,他引:3
1前言本文的第一部分分析了射流气体撞击限流沿后的发展过程以及射流入射角、限流沿高度等对二次射流气体发展情况的影响。本文将详细分析射流气体撞击限流沿后所形成的二次射流的速度和浓度的分布规律,并利用标量耗散率描述了射流气体的混合情况。众所周知,混合是扩散火焰燃烧速度的控制因素。通常扩散燃烧区内的温度足以使燃烧化学反应瞬间完成,因此燃烧时间完全取决于混合时间,即燃烧反应的速率由混合速率来控制。RW.Bilger等[1]认为扩散燃烧反应只有当完全达到分子级混合时才发生,他们在研究中利用标量耗散率概念来描述分子级混… 相似文献
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《物理学报》2017,(1)
采用耦合水平集-体积分数法并综合考虑传热及接触热阻作用建立了中空液滴碰撞水平壁面数值模型,并验证了模型的可靠性.通过分析计算结果,获得了中空液滴与实心液滴撞壁的动力学特征差异,揭示了中空液滴撞壁流动传热机理和中心射流形成机制,探索了碰撞速度和壁面浸润性对中空液滴撞壁动力学和传热特性的影响.研究表明:中空液滴撞壁后中心射流特征明显,并伴随有射流收缩和液壳破碎等现象.中空液滴内部压力梯度是液滴铺展、中心射流产生和发展的主要原因;撞壁过程中中心射流表面温度分布较为均匀,破碎液壳表面温度分布波动较大.碰撞速度与中空液滴撞壁最大铺展系数的相关性较小,但其对无量纲射流长度和壁面平均热流密度的影响较大;壁面浸润性与中空液滴撞壁后期铺展系数的相关性较大,但其对无量纲射流长度和壁面平均热流密度的影响较小. 相似文献
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《工程热物理学报》2020,(5)
本文基于多尺度液滴撞壁形态提出了新的考虑了不同飞溅状态的撞壁模型。结合容弹实验研究了近壁区域喷雾撞壁后火焰发展过程,对影响近壁区燃烧过程及碳烟生成规律的边界温度进行了探讨。结果表明,环境温度和壁面温度对喷雾撞壁后的液膜沉积量以及后续的燃烧过程影响显著。碳烟产生峰值直接和壁面燃油沉积量呈正相关,而较高的近壁区域温度可加速燃油蒸发并减少燃油沉积量。燃油沉积量的不同,其火焰发展形式不同:当沉积燃油较少时,近壁混合气形成较快,从而维持了稳定的燃烧过程;而当沉积燃油较多时,近壁区域的燃烧呈现不稳定的池火过程。随着环境温度和壁温的增加,油膜燃烧时刻提前并形成可燃混合气,从而加速了碳烟的生成和氧化。 相似文献
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本文将燃气轮机透平叶片压力面气膜冷却射流对端壁气膜冷却的影响作为研究对象,实验件表面绝热壁面气膜有效度通过压力敏感漆(Pressure Sensitive Paint)技术进行测量,在不同压力面和端壁气膜冷却吹风比条件下获得了端壁表面气膜有效度分布.实验结果表明压力面气膜冷却射流与端壁气膜冷却射流间存在相互干扰,端壁气膜射流在压力面气膜射流的影响下会出现明显偏移和再分布,尤其是端壁下游的气膜覆盖特性对压力面射流极为敏感.同时本文也定量分析了压力面射流的端壁效应,对当地气膜有效度分布进行了多个位置的对比和分析. 相似文献
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采用分子动力学模拟方法研究了表面力场对纳米通道内气体剪切流动的影响规律.结果显示通道内的气体流动分为两个区域:受壁面力场影响的近壁区域和不受壁面力场影响的主流区域.近壁区域内,气体流动特性和气体动力学理论预测差别很大,密度和速度急剧增大并出现峰值,正应力变化剧烈且各向异性,剪切应力在距壁面一个分子直径处出现突变.主流区域的气体流动特性与气体动力学理论预测相符合,该区域内的密度、正应力与剪切应力均为恒定值,速度分布亦符合应力-应变的线性响应关系.不同通道高度及密度下,近壁区域的归一化密度、速度及应力分布一致,表明近壁区域的气体流动特性仅由壁面力场所决定.随着壁面对气体分子势能作用的增强,气体分子在近壁区域的密度和速度随之增大,直至形成吸附层,导致速度滑移消失.通过剪切应力与切向动量适应系数(TMAC)的关系,得到不同壁面势能作用下的TMAC值,结果表明壁面对气体分子的势能作用越强,气体分子越容易在壁面发生漫反射. 相似文献
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We performed large-eddy simulations (LES) of forced impinging jets over smooth and rough surfaces, containing large-scale, azimuthal vortices generated by the enhanced primary instability in the jet shear layer. The interaction between these vortices and the turbulence in the wall jet that is formed downstream of the impingement region determines their rate of decay. To explore the surface-roughness effects on the evolution of the vortices, sand-grain-like surfaces are generated using uniformly distributed but randomly oriented ellipsoids. The flow is compared to our previous LES of jets impinging on a smooth surface. In spite of the severe modification caused by the roughness on the near-wall flow, the vortex development is not significantly altered. Slightly faster decay of the primary vortices is observed in the rough-wall case compared to the smooth-wall one; the secondary vortex that detaches from the wall and is lifted up has larger vorticity. The highly disturbed near-wall flow is advected outward and affects the evolution of the primary vortex for a longer period during the vortex interaction. The robust turbulent generation mechanism in the outer shear layer, however, mitigates the changes in vortex behaviour. The momentum deficit and the enhancement of turbulence due to the surface roughness play a key role during this process. 相似文献
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This is the second part of a survey summarizing authors’ research over a period of two decades on enhancing impinging jet
heat and/or mass transfer by periodic unsteadiness of nozzle flow rate. The first part, Tesař and Trávníček (2004 b), identified
the reasons why pulsation does not always improve the transfer rate: the pulses do not reach up to the wall. The authors nevertheless
demonstrate a transfer rate improvement, but in flows with inherent instability found in annular impinging jet. The excitation
there causes a topological metamorphosis (reversal of flow character). Also in the extreme case of the synthetic (zero time-mean
flow) jets the authors demonstrated a substantial improvement with the annular nozzle. The new approaches presented in the
paper offer increased performance of drying and heating/cooling systems, in particular in microdevices with otherwise low
or absent levels of natural jet turbulence. 相似文献
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Local heat transfer coefficients from a flat plate to a pair of circular air impinging jets are investigated experimentally, A pair of well-controlled, fully developed circular air impinging jets at room temperature are used in the experiments. The experimental method in this investigation is the transient liquid-crystal technique. During the experiments, the surface liquid-crystal color distribution of the test plate is recorded using a video imaging acquisition system, and the color information is translated into a surface temperature distribution through a digital color image processing unit. Local heat transfer coefficients art obtained using a surface transient heat conduction analysis. The flow Reynolds number of the jet is kept at 23,000. The jet-to-plate distance and the jet-to-jet spacing are varied in the experiment. Detailed radial heat transfer distributions at different radial directions are obtained and analyzed for L/D = 2, 4, 6, 8, and 10. The effect of jet spacing distance (S/D =1.75, 3.5,5.25, 7.0) is analyzed by comparing to data obtained from a single jet with similar flow configurations. 相似文献