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Cyclic variations of initial flame kernel growth in a Honda VTEC-E lean-burn spark-ignition engine

机译:本田VTEC-E稀薄火花点火发动机初始火焰核生长的循环变化

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Lean combustion in spark-ignition engines has long been recognized as a means of reducing both exhaust emissions and fuel consumption. However, problems associated with cycle-by-cycle variations in flame initiation and development limit the range of lean-burn operation. An experimental investigation was undertaken in order to quantify the effects of spark energy released and initial flame kernel growth on the cyclic variability of IMEP and crank angle at which 5% mass fraction was burned in a Honda VTEC-E, stratified- charge, pentroof-type, single-cylinder, optically accessed, spark-ignition engine. Simultaneous CCD images of the flame at the spark plug were acquired from two orthogonal views (one through the piston crown and one through the pentroof) on a cycle-by-cycle basis during the first 40 crank angle degrees after ignition timing, for isooctane port injection at an air to fuel ratio of 22, engine speed of 1500 RPM, 30% volumetric efficiency and 40° crank angle spark advance. The stage of the first 40° crank angle after ignition timing corresponded to the average time of 5% mass fraction burned. Image acquisition was synchronized with in-cylinder pressure, spark voltage and spark current sampling, for each of the following four spark-plug orientations: upstream, downstream and two crossflow positions of the ground electrode relative to the mean ensemble-averaged velocity vector at the spark-plug location at ignition timing. The measurements showed large cycle-by-cycle variations in flame size, shape and location. The flame size (projected enflamed areas through the two views and estimated enflamed volume) at 40° crank angle after ignition timing was found to correlate with coefficients as high as -0.96 with the crank angle of 5% mass fraction burned and 0.85 with IMEP. This degree of correlation between the flame size and the crank angle of 5% mass fraction burned or IMEP, reduced as the crank angle after ignition timing decreased, but correlations were still as large as -0.64 between the flame size at 10° crank angle after ignition timing and the crank angle of 5% mass fraction burned. The crossflow orientations produced the lowest levels of cyclic variability in IMEP, the upstream one the highest and the downstream orientation performed in between. The spark duration was found to vary from 12° to 22° crank angle on a cycle-by-cycle basis, being 19° crank angle on average, and this in conjunction with the behavior of the flame- size correlations with the crank angle of 5% mass fraction burned suggests that the "quality" of a cycle is determined within the short time of the spark discharge. High spark energies were generally associated with short durations of the spark event and always faster than average initial flame kernel growth cycles. The correlation coefficient between spark energy and flame volume was as high as 0.76 at 10° crank angle after ignition timing, decreasing to 0.59 at 20° crank angle after ignition timing. The displacement of the flame luminous center was not found to produce very strong correlation coefficients with the crank angle of 5% mass fraction burned (<0.55), but the correlations with the spark energy and, mainly, duration were quite strong (0.5-0.7), especially for the later stage of 20° crank angle after ignition timing rather than the earlier one of 10° crank angle after ignition timing. Although mostly associated with low spark energies, long spark durations could also produce fast cycles presumably because they provided an ignition window large enough to mask the effects of in-cylinder variations. For cycles with a given spark energy, the ones with the longest duration always produced higher than average initial flame kernel growth cycles.
机译:在火花点火发动机稀燃长期以来被认为是减少两个废气排放和燃料消耗的手段。然而,随着火焰萌生和发展的限制稀燃操作的范围内逐周期变化相关的问题。的实验研究是为了量化在IMEP和曲柄角度的循环变异在该5%质量分数的本田VTEC-E被​​烧掉了,分层充气,pentroof-火花能量释放和初始焰核增长的影响进行型,单汽缸,光学访问的,火花点火式发动机。在火花塞的火焰的同时CCD图像期间点火正时之后的前40度曲柄角,从上一个逐周期的基础两个正交视图(一个通过活塞顶和一个通过屋脊)获取,对异辛烷端口注射在空气22燃料比,1500 RPM,30%的容积效率和40°曲柄角的点火提前的发动机速度。点火正时之后的第一40°曲柄角的阶段对应于5%质量分数的平均时间燃烧。图像获取用缸内压力,火花电压和火花电流采样同步,对于每个下列四个火花塞取向:上游,下游,并在相对于平均整体平均速度矢量接地电极的2个横流位置在点火正时火花塞位置。测量表明在火焰尺寸,形状和位置的大周期接一个周期的变化。火焰尺寸(投影通过两个视图想象激怒区域和估计的想象激怒体积)在40°曲柄角后点火正时被发现关联具有系数高达-0.96用5%质量分数的曲柄角燃烧并与0.85 IMEP。这种程度的火焰大小和5%质量分数的曲柄角之间的相关性的烧毁或IMEP,减小曲轴转角之后点火正时降低,但相关性仍大到火焰大小之间-0.64以10°的曲轴角度后点火正时和5%质量分数的曲柄角烧毁。横流方向产生的循环变化的最低水平IMEP,上游一个最高和在之间执行的下游方向。火花持续时间被发现从上一个逐周期的基础上12°至22°的曲柄角度而变化,作为平均19°曲柄角,并且这在与的曲柄角的火焰大小相关的行为结合5%质量分数燃烧表明一个周期的“质量”是火花放电的很短的时间内被确定。高能量火花一般都与火花事件的持续时间短,总是比相关的平均初始火焰核生长周期快。火花能量和火焰容积之间的相关系数高达0.76在点火正时后10°曲轴转角,在点火正时后20°曲轴转角下降到0.59。火焰发光中心的位移未发现用5%质量分数的曲柄角度,以产生非常强的相关系数烧(<0.55),但与火花的能量,所述的相关性主要是,持续时间是相当强的(0.5-0.7 ),特别是对于20°曲柄角的点火正时,而不是点火正时之后的较早10°一个曲柄角后的稍后阶段。尽管大多与低能量火花相关联,长持续时间的火花也可能产生大概是因为它们提供了一种点火窗大到足以掩盖缸内变化的影响快速循环。对于具有给定火花能量循环中,具有最长持续时间的那些总是产生了比平均初始火焰核生长周期越高。

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