Leaner lifted-flame combustion with ducted fuel injection: The key role of forced two-stage mixing

被引:3
作者
Feng, Yizhuo [1 ]
Shang, Tansu [1 ,2 ]
Cai, Junqian [1 ]
Sun, Kai [1 ]
Wang, Tianyou [1 ]
机构
[1] Tianjin Univ, State Key Lab Engines, Tianjin 300350, Peoples R China
[2] State Key Lab Intelligent Agr Power Equipment, Luoyang 471039, Peoples R China
基金
中国国家自然科学基金;
关键词
Ducted fuel injection; Large eddy simulation; Two -stage mixing; Spray combustion; LARGE-EDDY SIMULATION; SPRAY INJECTION; SOOT FORMATION; IGNITION; TEMPERATURE;
D O I
10.1016/j.fuel.2023.128431
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
Ducted fuel injection (DFI) is a new approach to realize low-soot combustion for mixing-controlled ignition engines, while the underlying physics still remains inadequately understood. In this work, a high-fidelity LES of the combustion process with DFI was performed under engine-relevant conditions, with a particular interest in understanding the formation of the leaner lifted-flame combustion. Results show that, compared to free spray, both the ignition delay time and the quasi-steady flame lift-off length of DFI are prolonged, while the relative flame lift-off length from the duct outlet is shortened. The ignition process of DFI is typically two-staged in the mixture fraction space, which is fundamentally determined by the duct-forced, two-stage mixing process in the physical space. The mean soot volume fraction is synergistically controlled by the mixture fraction and the dissipation rate at the duct outlet and shows a nonmonotonic variation of "decrease-increase" with increasing duct length. To achieve leaner lifted-flame combustion, the duct outlet should pursue a balance between a globally rich (to avoid pre-ignition in the duct), spatially uniform (to avoid an excessively rich spray core) mixture and a certain large scalar dissipation rate (to extend the flame lift-off length). Compared to the conventional rich lifted flame of free spray, the leaner lifted flame structure of DFI exhibits a broader hightemperature-induced mode region, and the low-temperature flame is no longer circumferentially surrounded by the high-temperature flame. The decrease of the peak mixture fraction in the quasi-steady flame avoids soot formation especially under high-dissipation-rate conditions, and a conceptual model is presented to describe key features of DFI.
引用
收藏
页数:12
相关论文
共 62 条
  • [1] Beale JC, 1999, ATOMIZATION SPRAY, V9, P623
  • [2] ON REDUCED MECHANISMS FOR METHANE AIR COMBUSTION IN NONPREMIXED FLAMES
    BILGER, RW
    STARNER, SH
    KEE, RJ
    [J]. COMBUSTION AND FLAME, 1990, 80 (02) : 135 - 149
  • [3] Direct numerical simulation of a temporally evolving air/n-dodecane jet at low-temperature diesel-relevant conditions
    Borghesi, Giulio
    Krisman, Alexander
    Lu, Tianfeng
    Chen, Jacqueline H.
    [J]. COMBUSTION AND FLAME, 2018, 195 : 183 - 202
  • [4] Soot formation modelling for n-dodecane sprays using the transported PDF model
    Chishty, Muhammad A.
    Bolla, Michele
    Hawkes, Evatt R.
    Pei, Yuanjiang
    Kook, Sanghoon
    [J]. COMBUSTION AND FLAME, 2018, 192 : 101 - 119
  • [5] Conway G., 2020, Transportation Engineering, V5, DOI DOI 10.1016/J.TRENG.2021.100080
  • [6] Understanding the ignition mechanism of high-pressure spray flames
    Dahms, Rainer N.
    Paczko, Guenter A.
    Skeen, Scott A.
    Pickett, Lyle M.
    [J]. PROCEEDINGS OF THE COMBUSTION INSTITUTE, 2017, 36 (02) : 2615 - 2623
  • [7] Dec J.E., 1997, SAE Transactions, V106, P1319
  • [8] Dec JE, 2001, SAE TECHNICAL PAPER, P1295
  • [9] Engine combustion network, COMBUSTION RES FACIL
  • [10] Federico Millo CS, 2021, SAE TECHNICAL PAPER, P15