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Experimental study on the two-phase flow pattern and transformation characteristics of a flow mixing nozzle under a moderate flow rate

机译:温度流速下流动混合喷嘴两相流动模式及变换特性的实验研究

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摘要

A flow mixing nozzle can produce satisfactory atomization for heavy oil. However, the study of the internal flow pattern of this nozzle, along with the spray morphology and its transformation, is currently limited to a low flow rate for the two-phase inlet. A flow mixing nozzle with a moderate inlet flow rate and various nozzle structures (H/D) was experimentally studied using a self-designed flow mixing nozzle and a self-constructed experimental platform, as described in this paper. The results demonstrate that at a moderate two-phase inlet flow rate, a clear cone is observed inside the nozzle that can be described by the cone angle and the dimensionless cone area. In short, as air inlet flow rate increases, the cone volume decreases, the jet atomization effect is enhanced, the distribution range narrows, the flow pattern changes to flow blurring, and the variation trend is the opposite of that when the water inlet flow rate is increased. An analysis of the experimental results demonstrate that the flow pattern and spray morphology of the flow mixing nozzle under a moderate inlet flow rate are determined by the inertial force of air and the inertial force and surface tension force of water. When the air flow rate is increased, the inertial force is enhanced, and the cone radial concavity is strengthened; or, the cone disappears. At this time, the spray morphology is mainly expressed as atomization. When the water flow rate increases, the water inertial force increases, and the cone changes to a radial protrusion. The spray morphology is mainly expressed as a jet or breakup.
机译:流动混合喷嘴可为重油产生令人满意的雾化。然而,该喷嘴的内部流动模式以及喷雾形态及其转化的研究目前限于两相入口的低流速。通过本文所述,通过自行设计的流动混合喷嘴和自构造的实验平台进行具有中等入口流速和各种喷嘴结构(H / D)的流动混合喷嘴。结果表明,在适度的两相入口流速下,在喷嘴内观察到透明锥形,其可以由锥角和无量纲锥形区域描述。简而言之,随着空气入口流量的增加,锥体体积降低,喷射雾化效果得到增强,分配范围变窄,流动模式变化为流动模糊,并且变化趋势与进水流速相反增加了。实验结果的分析表明,在中等入口流速下流动混合喷嘴的流动模式和喷雾形态由空气的惯性力和水的惯性力和表面张力和表面张力决定。当空气流速增加时,提高惯性力,并强化锥形径向凹陷;或者,锥体消失了。此时,喷雾形态主要表示为雾化。当水流量增加时,水惯性力增加,并且锥体变为径向突出。喷雾形态主要表示为喷射或分析。

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