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Frontiers in Energy

ISSN 2095-1701

ISSN 2095-1698(Online)

CN 11-6017/TK

邮发代号 80-972

2019 Impact Factor: 2.657

Frontiers in Energy  2016, Vol. 10 Issue (2): 164-175   https://doi.org/10.1007/s11708-016-0407-9
  本期目录
Assessment and validation of liquid breakup models for high-pressure dense diesel sprays
Yi REN,Xianguo LI()
Department of Mechanical and Mechatronics Engineering, University of Waterloo, Waterloo, Ontario, Canada
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Abstract

Liquid breakup in fuel spray and atomization significantly affects the consequent mixture formation, combustion behavior, and emission formation processes in a direct injection diesel engine. In this paper, different models for liquid breakup processes in high-pressure dense diesel sprays and its impact on multi-dimensional diesel engine simulation have been evaluated against experimental observations, along with the influence of the liquid breakup models and the sensitivity of model parameters on diesel sprays and diesel engine simulations. It is found that the modified Kelvin-Helmholtz (KH)–Rayleigh-Taylor (RT) breakup model gives the most reasonable predicted results in both engine simulation and high-pressure diesel spray simulation. For the standard KH-RT model, the model constant Cbl for the breakup length has a significant effect on the predictability of the model, and a fixed value of the constant Cbl cannot provide a satisfactory result for different operation conditions. The Taylor-analogy-breakup (TAB) based models and the RT model do not provide reasonable predictions for the characteristics of high-pressure sprays and simulated engine performance and emissions.

Key wordsbreakup model    diesel engine    high-pressure injection    simulations
收稿日期: 2015-08-12      出版日期: 2016-05-27
Corresponding Author(s): Xianguo LI   
 引用本文:   
. [J]. Frontiers in Energy, 2016, 10(2): 164-175.
Yi REN,Xianguo LI. Assessment and validation of liquid breakup models for high-pressure dense diesel sprays. Front. Energy, 2016, 10(2): 164-175.
 链接本文:  
https://academic.hep.com.cn/fie/CN/10.1007/s11708-016-0407-9
https://academic.hep.com.cn/fie/CN/Y2016/V10/I2/164
Engine Caterpillar 3401E single cylinder oil test engine (SCOTE)
Bore×stroke/mm 137.2 ×165.1
Compression ratio 16.1:1
Displacement/L 2.44
Connecting rod length/mm 261.6
Squish height/mm 1.57
Intake valve closing/(°) ATDC –143
Exhaust valve opening/(°) ATDC 130
Tab.1  
Injector type Electronic unit injector (EUI)
Maximum injection pressure/MPa 190
Number of nozzle holes 6
Nozzle hole diameter/mm 0.214
Included spray angle 130˚
Injection rate shape Rising
Tab.2  
Fig.1  
Physical process Model
Drop collision NTC model [11]
Drop turbulent dispersion O’Rourke turbulent dispersion model
Drop vaporization Amsden-Chiang model [23]
Ignition and combustion (Only used in the engine simulation) Shell+characteristic time combustion (CTC) model [24]
Pollutant formation (Only used in the engine simulation) Extended Zel’dovich model &Hiroyasu-NS coxidation soot model [25,26]
Tab.3  
Fig.2  
Injection pressure/MPa Injection duration/ms Ambient temperature/K Ambient density/(kg·m–3) Injector diameter Dn/mm
180 1.0 950 60 0.1
Tab.4  
Case Breakup Model
1 KH-RT modified model
2 KH-RT model with the breakup length constant Cbl=10 in Eq. (20)
3 KH-RT model with Cbl=20 in Eq. (20)
4 KH-RT model with Cbl=40 in Eq. (20)
5 TAB model (without the drop size distribution)
6 TAB-CHI model (with the chi-squared drop size distribution)
7 TAB-RR model (with the Rosin-Rammler drop size distribution)
Tab.5  
Fig.3  
Fig.4  
Fig.5  
Fig.6  
Fig.7  
Engine speed Start of injection/(˚) ATDC Injection duration EGR/% Intake pressure/kPa Intake temperature/K
821 –9 5.5˚ 48.34 103 393
Tab.6  
Fig.8  
Fig.9  
Fig.10  
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