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Twin-Peak Heat Release Phenomenon Inside a Heavy-Duty Diesel Engine Retrofitted to Natural-Gas Spark Ignition

机译:改装为天然气火花点火的重型柴油发动机内部的双峰放热现象

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Existing compression ignition engines can be modified to spark ignition configuration to increase the use of natural gas in the heavy-duty transportation sector. A better understanding of the premixed natural gas combustion inside the original diesel chamber (i.e., flat-head-and-bol-in-piston) will help improve the conversion process and therefore accelerate the diesel engine conversion. Previous studies indicated that the burning process in such engines is a two-stage combustion with a fast burning inside the bowl and a slower burning inside the squish. This paper used experimental and numerical results to investigate the combustion process at a more advanced spark timing representative of ultra-lean medium-load operation, which placed most of the combustion inside the compression stroke. At such operating conditions, the high turbulence intensity inside the squish region accelerated the flame propagation inside the squish region to the point that the burn inside the bowl separated less from that inside the squish region. However, several individual cycles produced a double-peak energy-release with the peak locations closer to the only one heat release peak seen in the average cycle. Moreover, RANS CFD simulations indicated that the time at which the flame entered the squish region was near the peak location of the energy-release process for the conditions investigated here. As a result, the data suggests that the double-peak seen in the apparent heat release rate was the result of the cycle-by-cycle variation in the flame propagation.
机译:可以将现有的压缩点火发动机修改为火花点火配置,以增加重型运输领域中天然气的使用量。更好地了解原始柴油室内(即平头活塞和缸内活塞)内部的预混合天然气燃烧将有助于改善转换过程,从而加快柴油发动机的转换速度。先前的研究表明,此类发动机的燃烧过程是两阶段燃烧,其中碗内部燃烧较快,而壁球内部燃烧较慢。本文使用实验和数值结果研究了在更高级的火花正时(代表超稀薄中等负荷运行)下的燃烧过程,该过程将大部分燃烧置于压缩冲程内。在这样的操作条件下,在压榨区域内部的高湍流强度使火焰在压榨区域内部传播,以至于钵内的燃烧与压榨区域内部的燃烧分离的程度较小。但是,几个单独的循环产生了一个双峰能量释放,其峰值位置更接近平均循环中唯一的一个放热峰。此外,RANS CFD模拟表明,对于此处研究的条件,火焰进入挤压区域的时间接近能量释放过程的峰值位置。结果,数据表明,表观放热速率中出现的双峰是火焰传播的逐周期变化的结果。

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