Optical and numerical study on the effect of wall impingement on passive jet ignition characteristics of methane/air mixture

被引:5
|
作者
Zhang, Yixiao [1 ]
Ma, Xiao [1 ]
Mao, Jianshu [1 ]
Fang, Yuwen [1 ]
Jiang, Changzhao [2 ]
Wang, Zhi [1 ]
Shuai, Shijin [1 ]
机构
[1] Tsinghua Univ, State Key Lab Intelligent Green Vehicle & Mobil, Beijing 100084, Peoples R China
[2] Brunel Univ London, Mech & Aerosp Engn Dept, Uxbridge UB8 3PH, England
基金
中国国家自然科学基金;
关键词
Pre-chamber jet ignition; Wall impingement; Ignition zone; Stagnation effect; HEAT-TRANSFER; COMBUSTION; HYDROGEN; H-2/AIR; GAS;
D O I
10.1016/j.fuel.2024.131467
中图分类号
TE [石油、天然气工业]; TK [能源与动力工程];
学科分类号
0807 ; 0820 ;
摘要
Pre-chamber turbulent jet ignition is a promising high-efficiency combustion technique to achieve stable leanburn operation for spark-ignition engines. Wall impingement by a high momentum turbulent jet could exert a critical influence on jet ignition behavior. In this work, the passive jet ignition characteristics of premixed methane/air mixture under wall impinging condition was investigated based on optical experiments in a constant volume chamber and numerical simulations. Two ignition modes were found for flat wall impinging cases across a range of non-dimensional impinging distances (H/D) from 5.7 to 20. In mode 1, ignition initiates from near wall region. Under lean conditions of lambda = 1.3, compared with that in the free jet case, the ignition delay time characterized by a 5 % mass fraction burned (MFB-05), decreases by 3.3 ms at H = 30 mm and increases by up to 6.6 ms at H = 20 mm. In mode 2, ignition initiates from the jet root. The ignition delay times are shorter for all impinging distances (H = 20, 30, 40 mm), with MFB-05 decreasing by up to 3.4 ms. Simulations reveal that when the wall is located in the jet developing zone with H/D below 7, wall impinging deteriorates the ignition, which is attributed by higher turbulent kinetic energy (TKE) and lower Damko<spacing diaeresis>hler (Da) number near the stagnation zone, resulting in extended ignition delay. Conversely, as H/D increases, ignition is promoted by the stagnation effect with a shorter ignition delay. Additionally, the effect of wall shapes was analyzed. Using sharp-tip V-shaped wall, the stagnation region with high TKE is minimized. A blunt-tip V-shaped wall shows enhanced impinging but no obvious increase of Da number at stagnation point. Using M-shaped wall, the ignition mode with a "lift-off" flame was found. Besides, ignition is more favorable in the secondary jet zone with active radicals and higher Da number.
引用
收藏
页数:19
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