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Research Article

Research on destructive knock combustion mechanism of heavy-duty diesel engine at low temperatures

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Received 25 Sep 2022, Accepted 05 Dec 2022, Published online: 16 Dec 2022
 

ABSTRACT

To clarify the mechanism of destructive knock combustion and piston ablation in heavy-duty diesel engines operating at low temperatures, CONVERGE simulation and wall temperature measurement were performed. The results show that as the initial temperature (intake valve closing instant) decreases from 380K to 307K, the spray wet-wall ratio increases from 12.8% to 22.2%. The fuel film evaporates slowly at low temperature before the hot flame, so the ignition is seriously delayed until the fuel injection ends, and the free-jet autoignition shifts to wall-attached combustion. However, the fuel film evaporation reverses after hot flame, and the maximum evaporation rate at 307K is about 54 times that at 380K. The wall temperature rises sharply to 350-450°C during wall-attached combustion. As the initial temperature decreases, the maximum pressure rise rate increases from 0.9MPa/°CA to 8.3MPa/°CA, and the pressure waves repeatedly oscillate along the end-center-end path in the cylinder. The highest pressure at the monitoring point is nearly an order of magnitude higher than the average, and the oscillation amplitude is as high as 6-10MPa, which far exceeds the failure threshold. The piston whose strength has been greatly reduced after thermal shock quickly undergoes ablation damage under strong pressure shock.

GRAPHICAL ABSTRACT

Highlights

  • Knock mechanism of heavy-duty diesel engines at low temperatures are clarified.

  • Fuel film evaporates slowly before hot flame at low temperatures but then reverses.

  • Free autoignition shifts to wall-attached combustion with decreasing temperature.

  • Pressure oscillation amplitude exceeds 6MPa with intake air temperature below 15°C.

  • Local high temperature and pressure shock together cause piston damage.

Acknowledgement

This work is supported by the National Natural Science Foundation of China (Grant Nos. 52176098), and the Project funded by China Postdoctoral Science Foundation (Grant No. 2021M700013). Any opinions, findings, and conclusions or recommendations expressed in this publication are those of the authors and do not necessarily reflect the views of the National Science Foundation and China Postdoctoral Science Foundation. The authors would like to thank the editors and reviewers for their valuable comments on this research.

Disclosure statement

No potential conflict of interest was reported by the authors.

Nomenclature

CVCC=

constant volume combustion chamber

FFT=

Fast Fourier transform

HRR=

heat release rate

HTI=

high-temperature ignition

HTR=

high-temperature region

LTI=

low-temperature ignition

PRR=

pressure rise rate

RWT=

return water temperature

SOI=

start of injection

Pinj=

injection pressure

dtinj=

injection duration

Lw=

wall distance

Tw=

initial wall temperature

PPmax=

maximum pressure oscillation amplitude

φ=

equivalence ratio

init_T=

initial temperature in the cylinder

Additional information

Funding

The work was supported by the China Postdoctoral Science Foundation [2021M700013]; National Natural Science Foundation of China [52176098]

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