期刊论文详细信息
FUEL 卷:299
An experimental and one-dimensional modeling analysis of turbulent gas ejection in pre-chamber engines
Article
Garcia-Oliver, J. M.1  Niki, Y.2  Rajasegar, R.3  Novella, R.1  Gomez-Soriano, J.1  Martinez-Hernandiz, P. J.1  Li, Z.3  Musculus, M. P. B.3 
[1] Univ Politecn Valencia, CMT Motores Term, Camino Vera, Valencia 46022, Spain
[2] Natl Inst Maritime Port & Aviat Technol, Tokyo 1810004, Japan
[3] Sandia Natl Labs, Livermore, CA USA
关键词: Pre-chamber spark ignition;    1-D gas jet model;    cycle-to-cycle variability;    infrared imaging;    high-speed visualization;   
DOI  :  10.1016/j.fuel.2021.120861
来源: Elsevier
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【 摘 要 】

Experimental results from a study on the evolution of gas jets ejected through the orifices of a pre-chamber in a heavy-duty optical engine are presented. The work examines conditions without fuel inside the main-chamber, which helps to describe the dynamics of the ejected gas jets without the interference of subsequent combustion in the main-chamber. Experimental diagnostics consist of high-speed visible intensified imaging and low-speed infrared imaging. Additionally a one-dimensional gas jet model is used to characterize the spatial distribution of the ejected flow, including parameters such as tip penetration, which are then validated based on experimental results. Different stages in the ejection of pre-chamber jets are identified, with chemical activity restricted to a maximum distance of 5 to 10 orifice diameters downstream of the orifice as indicated by the recorded visible radiation. Sensitivity of cycle-to-cycle variations in pre-chamber jet development to the air-to-fuel ratio in the pre-chamber observed in the experiments is in most part attributed to the variations in the timing of combustion initiation in the pre-chamber. The influence of the ejection flow on the penetration of the gas jet on a cycle-tocycle basis is presented using the one-dimensional model. The one-dimensional model also indicates that the local flow exhibits highest sensitivity to operating conditions during the start of ejection until the timing when maximum flow is attained. Differences that exist during the decreasing mass-flow ejection time-period tend to smear out in part due to the transient slowdown of the ejection process.

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