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首页> 外文期刊>Atomization and Sprays: Journal of the International Institutes for Liquid Atomization and Spray Systems >Experimental Investigation of the Drop Size Distribution of Sprays Produced by A Low-Velocity Netwonian Cylindrical Liquid Jet
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Experimental Investigation of the Drop Size Distribution of Sprays Produced by A Low-Velocity Netwonian Cylindrical Liquid Jet

机译:低速Netwonian圆柱液体射流产生的喷雾液滴尺寸分布的实验研究

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摘要

The origin of the critical point of a cylindricalliquidjet,first maximum of the stability CUMIe, is not fully understood so far. In a previoUs experimental investigation, three different jet regimes of atomization were defined according to the influence of the gas density on the jet critical velo- city. Whether a jet is in a given regime was found to be a function of a parameter Pa 0, equiva- lent to a density. In the present investigation, the relevance of this parameter is considered and jet atomization processes are studied through the analysis of the evolution of the drop size distri- bution in the vicinity of the critical condition. A (Pa 0, Z) map is derived from the analysis of a large amount of experimental results found in the literature. This map is of practical interest, as it helps in presupposing the behavior of a liquid jet. The analysis of the drop size distribution reveals that the instability that develops when the critical velocity is reached may be a subcritical or a supercritical instability, according to the jet regime of atomization. When a subcritical instability develops, the disintegration process is controlled by capillary instability even for velocities greater than the critical velocity, and the breakup length varies according to the initial conditions. It was found that the develop- ment of such instabilities has no effect on the relative drop size distribution width, 'Which seems therefore to be mainly a function of the perturbation growth process. When a supercritical insta- bility develops, the development of the criticalpointis due to the action of the aerodynamicforces, 'Which increases the temporalgrowth rate of the instability as the velocity increases.
机译:到目前为止,圆柱状液体射流的临界点的起点,即稳定性CUMIe的第一个最大值,尚不完全清楚。在先前的实验研究中,根据气体密度对喷射临界速度的影响,定义了三种不同的雾化喷射方式。发现射流是否处于给定状态是参数Pa 0的函数,该参数等于密度。在本研究中,考虑了该参数的相关性,并通过分析临界条件附近液滴尺寸分布的演变来研究射流雾化过程。 (Pa 0,Z)图来自对文献中发现的大量实验结果的分析。该图具有实际意义,因为它有助于预设液体射流的行为。液滴尺寸分布的分析表明,根据雾化的喷射方式,达到临界速度时出现的不稳定性可能是亚临界或超临界不稳定性。当出现亚临界不稳定性时,即使对于大于临界速度的速度,崩解过程也受毛细管不稳定性的控制,并且破裂长度根据初始条件而变化。已经发现,这种不稳定性的发展对相对的液滴尺寸分布宽度没有影响,因此,这似乎主要是扰动生长过程的函数。当超临界不稳定发展时,临界点的发展是由于空气动力的作用,“随着速度的增加,不稳定的时间增长率会增加。

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