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Mixing in high Schmidt number turbulent jets

机译:混合高施密特数湍流喷射

摘要

NOTE: Text or symbols not renderable in plain ASCII are indicated by [...]. Abstract is included in .pdf document.ududThis thesis is an experimental investigation of the passive scalar (species concentration) field in the far-field of round, axisymmetric, high Schmidt number (liquid phase), turbulent jets issuing into a quiescent reservoir, by means of a quantitative laser-induced fluorescence technique. Single-point concentration measurements are made on the jet centerline, at axial locations from 100 to 305 nozzle diameters downstream, and Reynolds numbers of 3,000 to 102,000, yielding data with a resolved temporal dynamic range up to [...], and capturing as many as 504 large-scale structure passages. Long-time statistics of the jet concentration are found to converge slowly. Between 100 and 300 large-scale structure passages are required to reduce the uncertainty in the mean to 1%, or so. The behavior of the jet varies with Reynolds number. The centerline concentration pdf's become taller and narrower with increasing Re, and the normalized concentration variances correspondingly decrease with Re. The concentration power spectra also evolve with Re. The behavior of the spectral slopes is examined. No constant -1 (Batchelor) spectral slope range is present. Rather, in the viscous region, the power spectra exhibit log-normal behavior, over a range of scales exceeding a factor of 40, in some cases. The frequency of the beginning of this log-normal range scales like [...] (Kolmogorov scaling). Mixing in the far-field is found to be susceptible to initial conditions. Disturbances in the jet plenum fluid and near the nozzle exit strongly influence the scalar variance, with larger disturbances causing larger variances, i.e., less homogeneous mixing. The plenum/nozzle geometry also influences the variance. These effects of initial conditions persist for hundreds of diameters from the nozzle exit, over hundreds of large scales. Mixing in these jets differs from gas-phase, order unity Sc, jet mixing. At low to moderate Re, the higher Sc jet is less well mixed. The difference is less pronounced at higher Re. Flame length estimates imply either an increase in entrainment and/or an increase in molecular mixing, with increasing Re. Experimental considerations such as buoyancy and resolution are shown not to influence these results.ud
机译:注意:用[...]表示无法用纯ASCII呈现的文本或符号。 .pdf文件中包含摘要。 ud ud本论文是对圆形,轴对称,高施密特数(液相),湍流射流成静态的远场中的被动标量(物种浓度)场的实验研究。通过定量激光诱导的荧光技术。 daccess-ods.un.org daccess-ods.un.org在喷嘴的中心线上进行单点浓度测量,轴向位置在下游直径为100至305个喷嘴,雷诺数为3,000至102,000,产生解析的时间动态范围高达的数据,并捕获多达504个大型结构通道。射流浓度的长期统计数据发现收敛缓慢。需要100到300个大型结构通道,才能将平均值的不确定性降低到1%左右。射流的行为随雷诺数而变化。中心线浓度pdf随着Re的增加而变高和变窄,而标准化浓度方差随Re的增加而减小。浓度功率谱也随Re演化。检查频谱斜率的行为。不存在恒定的-1(Batchelor)光谱斜率范围。而是在某些情况下,在粘性区域中,功率谱在超过40倍的比例范围内显示出对数正态行为。该对数正态范围的开始频率像(Kolmogorov标度)一样标度。发现在远场混合容易受到初始条件的影响。喷射增压流体和喷嘴出口附近的扰动强烈地影响标量变化,较大的扰动引起较大的变化,即,较不均匀的混合。增压/喷嘴的几何形状也会影响变化。初始条件的这些影响在从喷嘴出口到数百个直径的数百个大尺度上持续存在。这些喷射中的混合不同于气相,顺序单一的Sc,喷射混合。在低至中等的Re下,较高的Sc射流混合得不太好。较高的Re时差异并不明显。火焰长度估计值意味着随着Re的增加,夹带增加和/或分子混合增加。实验结果表明浮力和分辨率等因素不会影响这些结果。 ud

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    Miller Paul Lewis;

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  • 年度 1991
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