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Using PIV Measurements to Determine the Role of the In-Cylinder Flow Field for Stratified DISI Engine Combustion

机译:使用PIV测量确定缸内流场对DISI发动机分层燃烧的作用

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In a companion study [1], experimental observations in a stratified-charge DISI engine operated with late injection of E70 led to the formation of two hypotheses: (1) For highly stratified spray-guided combustion, the heat-release rate of the main combustion phase is primarily controlled by mixing rates and turbulence level associated with fuel-jet penetration. (2) During the main combustion phase, the role of the in-cylinder flow field generated by the intake and compression strokes is primarily its stochastic disturbance of the mixing and flow associated with the fuel jets, thereby causing cycle-to-cycle variations of the spray-guided stratified combustion. Here, these hypotheses are tested. An optical engine was operated skip fired at 1000 and 2000 rpm, and exhibited the same combustion properties observed in the steady-state all-metal engine tests. High-speed particle image velocimetry (PIV) and spray imaging are used to quantify the intake-generated in-cylinder flow momentum, the spray induced momentum, and the resulting liquid spray variability. The PIV measurements reveal that the spatially-averaged gas-flow speed (momentum) without injection at 2000 rpm is twice that of 1000 rpm. In contrast, just after injection the gas flow spatial average speed at 2000 rpm is only 24% higher due to the dominance of spray momentum. This is comparable to the 16% increase of the measured ensemble-averaged heat-release rate (in kW). The cyclic variability of the in-cylinder flow speed prior to injection is measured to be considerably higher at 2000 rpm compared to 1000 rpm. Though the injected liquid spray reduced the flow-speed cyclic-variability after injection, the higher variability did persist. The spray imaging reveals that the increased flow-speed variability at 2000 rpm causes increased variability of the spray jet trajectory, jet coalescence, and spray rotation from cycle to cycle. This work supports both the hypotheses that motivated this study.
机译:在一项伴随研究中[1],在分层喷射DISI发动机上进行E70后期喷射操作的实验观察结果形成了两个假设:(1)对于高度分层的喷雾引导燃烧,主发动机的放热率燃烧阶段主要由与燃油喷射渗透相关的混合速率和湍流水平控制。 (2)在主燃烧阶段,由进气冲程和压缩冲程产生的缸内流场的作用主要是其与燃料喷射流相关的混合和流动的随机扰动,从而导致燃料的循环变化。喷雾引导分层燃烧。在这里,对这些假设进行了检验。光学引擎以1000 rpm和2000 rpm的速动进行操作,并表现出在稳态全金属引擎测试中观察到的相同燃烧特性。高速粒子图像测速(PIV)和喷雾成像用于量化进气产生的缸内流动动量,喷雾引起的动量以及由此产生的液体喷雾可变性。 PIV测量表明,在2000 rpm时不注入的空间平均气体流速(动量)是1000 rpm的两倍。相反,在刚注入后,由于喷雾动量的优势,气流在2000 rpm时的空间平均速度仅高出24%。这相当于测量的整体平均放热率(以kW为单位)增加了16%。在注入之前,缸内流速的周期性变化在2000 rpm时测得明显高于1000 rpm。尽管注入的液体喷雾降低了注入后的流速循环变异性,但较高的变异性仍然存在。喷雾成像显示,在2000 rpm时增加的流速可变性会导致喷雾喷射轨迹,喷射聚结和喷雾循环之间的旋转性增加。这项工作支持了促使这项研究的两种假设。

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