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Journal of ZheJiang University (Engineering Science)  2025, Vol. 59 Issue (2): 394-401    DOI: 10.3785/j.issn.1008-973X.2025.02.017
    
Dynamic evolution of soot particle growth in diesel engine cylinder
Yuanxin YU1,2(),Mingrui WEI1,2,Hongling JU1,2,*()
1. Hubei Provincial Key Laboratory of Modern Auto Parts Technology, Wuhan University of Technology, Wuhan 430070, China
2. Auto Parts Technology Hubei Provincial Collaborative Innovation Center, Wuhan University of Technology, Wuhan 430070, China
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Abstract  

A three-dimensional simulation model was established by taking an in-cylinder direct-injection diesel engine as the prototype. A detailed soot model was coupled to analyze the mass distribution and number density variation of soot particles in the cylinder of the diesel engine under different load. The calculated results and airflow parameters were taken as the initial conditions for dynamic simulation, and the particle dynamics model was established by using the Lagrange method to track the motion of each particle in order to calculate the complete growth process of soot particles. Results showed that the nucleation rate of soot gradually approaches zero, the surface growth and condensation rate were lower than the oxidation rate, and the total mass of soot gradually decreased after combustion. The soot mass fraction at the top of the cylinder, cylinder wall, and piston was relatively low. The constructed particle dynamics model can simulate the growth process from basic particles of soot to aggregates. The particle dynamics model can be used to simulate the growth process from soot elementary particles to aggregates, and the morphology of the aggregates obtained under different loads was mainly branched and clustered structure, which was similar to the main morphologies obtained by experimental sampling. The fractal dimensions under different loads were similar to those measured by the experiments, with a maximum error of about 1.5%.



Key wordsdiesel engine      soot particle      detailed soot model      dynamic evolution      morphology      fractal dimension     
Received: 22 December 2023      Published: 11 February 2025
CLC:  TK 42  
Fund:  国家自然科学基金资助项目(51706163).
Corresponding Authors: Hongling JU     E-mail: 1786198559@qq.com;juhongling@whut.edu.cn
Cite this article:

Yuanxin YU,Mingrui WEI,Hongling JU. Dynamic evolution of soot particle growth in diesel engine cylinder. Journal of ZheJiang University (Engineering Science), 2025, 59(2): 394-401.

URL:

https://www.zjujournals.com/eng/10.3785/j.issn.1008-973X.2025.02.017     OR     https://www.zjujournals.com/eng/Y2025/V59/I2/394


柴油机缸内碳烟颗粒生长的动力学演变

以一台缸内直喷柴油机为原型,建立三维仿真模型,耦合详细碳烟模型,研究柴油机在不同负荷下缸内碳烟颗粒的质量分布和数密度变化规律. 将计算得到的结果及气流参数作为动力学模拟的初始条件,利用拉格朗日方法建立颗粒动力学模型追踪每个颗粒的运动,计算碳烟颗粒的完整生长过程. 结果表明,燃烧结束后,碳烟成核速率逐渐趋近于零,表面生长和凝结速率低于氧化速率,碳烟总质量逐渐降低;气缸顶部、气缸壁及活塞处的碳烟质量分数均较小. 利用构建的颗粒动力学模型,可以模拟碳烟基本粒子到团聚体的生长过程,在不同负荷下得到的积聚体形貌主要呈枝状和簇状结构,与实验采样得到的几种主要形貌相似;不同负荷下的分形维数均与实验测量值相近,最大误差约为1.5%.


关键词: 柴油机,  碳烟颗粒,  详细碳烟模型,  动力学演变,  形貌,  分形维数 
Fig.1 Flowchart of particle collision calculation
参数数值
发动机类型四缸四冲程
缸径/mm96
行程/mm103
排量/L2.982
压缩比17.5
标定功率/kW85
标定转速/(r·min?13200
连杆长度/mm155
喷孔数7
Tab.1 Main parameter of diesel engine (YC4FA 116-40)
Fig.2 Schematic of combustion chamber mesh
模拟类型模型
湍流模型RNG k-ε
蒸发模型Frossling
碰撞模型NTC collision
破碎模型KH-RT
燃烧模型SAGE
碳烟模型Particle Size Mimic
NOx模型Extended Zeldovich
Tab.2 Mathematical model in three-dimensional simulation
Fig.3 Comparison of simulation and experimental value of cylinder pressure and heat release rate
Fig.4 Soot mass fraction in cylinder under different load
Fig.5 Soot number density at top of cylinder
Fig.6 Average number density and total mass of soot at 50% load
Fig.7 Mass change in soot nucleation, surface growth, condensation and oxidation at 50% load
Fig.8 Total mass fraction of soot in cylinder at different time under 50% load
p /MPavg/(m·s?1)k/(m2·s?2)?/ (m2·s?3)
0.184.410.757206.71
0.384.400.766153.75
0.635.171.082275.89
0.886.401.089260.02
1.139.221.501294.43
Tab.3 Airflow parameter at different load
参数数值
ρp/(g·cm?3)1.8
A/ J1×10?19
e0.4
${z_0}$/ m4×10?10
${{{{{p}}}} _{\text{pl}}}$/ Pa5×109
${u_{\text{f}}}$0.4
Tab.4 Particle property in turbulence
Fig.9 Initial spatial distribution map of particles in computational domain
Fig.10 Cross-sectional view of calculation domain at beginning of calculation under 50% load
Fig.11 Cross-sectional view of calculation domain at end of calculation under 50% load
Fig.12 Schematic diagram of soot particle accumulation at end of calculation
Fig.13 Actual soot accumulation morphology [21]
Fig.14 Changing trend of soot particle fractal dimension
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