首页> 外文会议>CSPE-JSME-ASME International Conference on Power Engineering Vol.1 Oct 8-11, 2001, Xi'an, China >DISTINCTIVE BURNING RATE OF DIESEL LIGHT OIL AND LIGHT CYCLE OIL DROPLETS
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DISTINCTIVE BURNING RATE OF DIESEL LIGHT OIL AND LIGHT CYCLE OIL DROPLETS

机译:柴油和轻循环油的区别燃烧率

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This study is devoted to testing the single droplet combustion of a diesel light oil (LO) and a light cycle oil (LCO). The tests were carried out in an atmospheric hot chamber preset at a temperature of 1173 K. A quartz fiber was used to suspend the oil droplet. The results showed that the LCO droplet had higher soot yield, whereas both the LCO and LO droplets did not have obvious coke formation. Microexplosions were obvious during the combustion but the LO droplets were more apt to microexplode. The ignition delay was relatively shorter for the LCO droplet but the flame lifetime and droplet lifetime were nearly the same for the droplets of both the oils (flame lifetime being the time between ignition and extinction, and droplet lifetime being the sum of ignition delay and flame lifetime). The disruptive burning more or less complicated the time-series variations of droplet size (d). A linear region, however, can still be identified on the curve d~2 vs. t to show the overall changes of droplet size with burning time (t). This allowed an apparent burning rate constant to be defined according to the d~2-law. The burning rate constant varied with the initial droplet diameter (d_0), which caused the relative droplet size, (d/d_0)~2, to be normalized by the relative time t/d_0~n (n=1.10). Further analysis showed that this normalization resulted from the respective unification of the unsteady and quasi-steady burning phases of different droplets. These results were also corroborated by burning an oil blend of LO and LCO at volume fractions of 50% in the same conditions.
机译:这项研究致力于测试柴油轻油(LO)和轻循环油(LCO)的单滴燃烧。该测试在预设温度为1173 K的大气热室中进行。使用石英纤维悬浮油滴。结果表明,LCO液滴的烟灰产率较高,而LCO和LO液滴均没有明显的焦炭形成。燃烧过程中微爆明显,但LO液滴更易于微爆。 LCO液滴的点火延迟相对较短,但两种油的液滴的火焰寿命和液滴寿命几乎相同(火焰寿命是点火和熄灭之间的时间,液滴寿命是点火延迟和火焰的总和。一生)。破坏性燃烧或多或少地使液滴尺寸(d)的时间序列变化复杂化。但是,仍可以在d〜2与t的关系曲线上确定一个线性区域,以显示液滴大小随燃烧时间(t)的总体变化。这允许根据d〜2定律定义表观燃烧速率常数。燃烧速率常数随初始液滴直径(d_0)而变化,这导致相对液滴尺寸(d / d_0)〜2通过相对时间t / d_0〜n(n = 1.10)进行归一化。进一步的分析表明,这种归一化是由于不同液滴的非稳态和准稳态燃烧相的统一所致。通过在相同条件下燃烧体积分数为50%的LO和LCO的油混合物也证实了这些结果。

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