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Characteristics of spray from a GDI fuel injector for naphtha and surrogate fuels

机译:GDI喷油器喷射的石脑油和替代燃料的喷雾特性

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Characterization of the spray angle, penetration, and droplet size distribution is important to analyze the spray and atomization quality. In this paper, the spray structure development and atomization characterization of two naphtha fuels, namely light naphtha (LN) and whole naphtha (WN) and two reference fuel surrogates, i.e. toluene primary reference fuel (TPRF) and primary reference fuel (PRF) were investigated using a gasoline direct injection (GDI) fuel injector. The experimental setup included a fuel injection system, a high-speed imaging system, and a droplet size measurement system. Spray images were taken by using a high-speed camera for spray angle and penetration analysis. Sauter mean diameter, Dv(10), Dv (50), Dv(90), and particle size distribution were measured using a laser diffraction technique. Results show that the injection process is very consistent for different runs and the time averaged spray angles during the measuring period are 103.45 degrees, 102.84 degrees, 102.46 degrees and 107.61 degrees for LN, WN, TPRF and PRF, respectively. The spray front remains relatively flat during the early stage of the fuel injection process. The peak penetration velocities are 80 m/s, 75 m/s, 75 m/s and 79 m/s for LN, WN, TPRF and PRF, respectively. Then velocities decrease until the end of the injection and stay relatively stable. The transient particle size and the time-averaged particle size were also analyzed and discussed. The concentration weighted average value generally shows higher values than the arithmetic average results. The average data for WN is usually the second smallest except for Dv90, of which WN is the biggest. Generally the arithmetic average particle sizes of PRF are usually the smallest, and the sizes does not change much with the measuring locations. For droplet size distribution results, LN and WN show bimodal distributions for all the locations while TPRF and PRF shows both bimodal and single peak distribution patterns. The results imply that droplet size distribution is skewed to the larger side for locations close the axis and is skewed to the smaller side for distance away from the axis. (C) 2016 Elsevier Ltd. All rights reserved.
机译:喷雾角度,穿透力和液滴尺寸分布的特征对于分析喷雾和雾化质量很重要。本文研究了轻质石脑油(LN)和全石脑油(WN)这两种石脑油燃料的喷雾结构发展和雾化特性,以及甲苯主要参考燃料(TPRF)和主要参考燃料(PRF)这两种参考燃料替代品。使用汽油直喷(GDI)燃油喷射器进行了研究。实验装置包括燃料喷射系统,高速成像系统和液滴尺寸测量系统。通过使用高速相机拍摄喷雾图像以进行喷雾角度和渗透性分析。使用激光衍射技术测量Sauter平均直径,Dv(10),Dv(50),Dv(90)和粒度分布。结果表明,不同过程的喷射过程非常一致,测量期间LN,WN,TPRF和PRF的时间平均喷雾角分别为103.45度,102.84度,102.46度和107.61度。在燃料喷射过程的早期,喷雾前沿保持相对平坦。 LN,WN,TPRF和PRF的峰值穿透速度分别为80 m / s,75 m / s,75 m / s和79 m / s。然后速度降低直到注射结束并保持相对稳定。还分析和讨论了瞬时粒度和时间平均粒度。浓度加权平均值通常显示出比算术平均值更高的值。除了Dv90以外,WN的平均数据通常第二少,其中WN最大。通常,PRF的算术平均粒径通常最小,并且粒径不会随测量位置变化太大。对于液滴尺寸分布结果,LN和WN显示所有位置的双峰分布,而TPRF和PRF显示双峰和单峰分布模式。结果表明,液滴尺寸分布在靠近轴的位置偏向较大的一侧,而在远离轴的距离偏向较小的一侧。 (C)2016 Elsevier Ltd.保留所有权利。

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