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Optical diagnostics on the pre-chamber jet and main chamber ignition in the active pre-chamber combustion (PCC)

机译:在主动预室燃烧(PCC)中的预室喷射和主腔点点火上的光学诊断(PCC)

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We studied the relationship between pre-chamber jet and main chamber ignition in the pre-chamber combustion (PCC) of an optical engine, fueled with methane and equipped with an active pre-chamber with two rows of orifices. Acetone planar laser-induced fluorescence (PLIF) and OH* chemiluminescence imaging techniques were simultaneously applied to visualize the pre-chamber jet and the reaction zone in the main chamber, respectively. The pre-chamber fueling was constant and the main chamber fueling was increased to form an ultra-lean case and a lean case with global excess air ratios (lambda) of 2.3 and 1.8, respectively. Results indicate that a higher pressure difference between pre-chamber and main chamber (AP) produces larger pre-chamber jet penetration speed; the maximum pre-chamber jet penetration speed appears at timing around the peak AP. Over enrichment of the pre-chamber charge reduces the peak AP and thus does not favor a faster pre-chamber jet discharge. In addition to the main pre-chamber jet, a weaker post jet discharge process is visualized; the former is due to the pre-chamber combustion while the latter due to the AP fluctuation and the cylinder volume expansion. The post pre-chamber jet is accompanied by a post reaction zone in the ultra-lean case (lambda= 2.3) and there are two unburned regions in the main chamber: one is around the pre-chamber nozzle and the other between the adjacent reaction zones. These two unburned regions are consumed by flame propagation in the lean case (lambda= 1.8). The weak pre-chamber jet from the upper-row orifice does not produce any distinct reaction zone, indicating that the pre-chamber orifice location and arrangement on the nozzle also matters in the pre-chamber design. The pre-chamber jet penetration length is longer than that of the reaction zone during pre-chamber discharge; the penetration length difference between the pre-chamber jet and reaction zone decreases with increasing main chamber fueling. (C) 2021 The Combustion Institute. Published by Elsevier Inc. All rights reserved.
机译:我们研究了在光学发动机的预室燃烧(PCC)中的预室射流和主腔点火之间的关系,用甲烷向配备有有两排孔口的活性预室。同时施加丙酮平面激光诱导的荧光(PLIF)和OH *化学发光成像技术以分别在主室中可视化预室射流和反应区。预室燃料是恒定的,并且增加主腔燃料以形成超瘦案例,并且分别具有2.3和1.8的全局过量空气比(Lambda)。结果表明,预室和主室(AP)之间的更高的压力差产生了更大的预室射流渗透速度;最大预室射流穿透速度在峰值AP周围的定时出现。在预腔电荷的富集中减少峰值AP,因此不利于更快的预室射流放电。除了主预室射流之外,还可视化较弱的后射流排放过程;前者是由于预腔燃烧,而后者由于AP波动和气缸体积膨胀。后预室射流伴随着超瘦壳体(Lambda = 2.3)中的后反应区,主腔室中有两个未燃烧的区域:一个是在腔室喷嘴周围和相邻反应之间的另一个区域。区域。这两个未燃烧的区域被瘦案例中的火焰传播消耗(Lambda = 1.8)。来自上排孔的弱预室射流不会产生任何不同的反应区,表明预室孔位置和在喷嘴上的布置也很重要。预室射流穿透长度在预室排出期间长于反应区的长度;预室射流和反应区之间的穿透长度差随着主室燃料的增加而降低。 (c)2021燃烧研究所。由elsevier Inc.保留所有权利发布。

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