Abstract
3D CFD spark-ignition IC engine simulations are extremely complex for the regular user. Truly-predictive CFD simulations for the turbulent flame combustion that solve fully coupled transport/chemistry equations may require large computational capabilities unavailable to regular CFD users. A solution is to use a simpler phenomenological model such as the G-equation that decouples transport/chemistry result. Such simulation can still provide acceptable and faster results at the expense of predictive capabilities. While the G-equation is well understood within the experienced modeling community, the goal of this paper is to document some of them for a novice or less experienced CFD user who may not be aware that phenomenological models of turbulent flame combustion usually require heavy tuning and calibration from the user to mimic experimental observations. This study used ANSYS® Forte, Version 17.2, and the built-in G-equation model, to investigate two tuning constants that influence flame propagation in 3D CFD SI engine simulations: the stretch factor coefficient, Cms and the flame development coefficient, Cm2. After identifying several Cm2-Cms pairs that matched experimental data at one operating conditions, simulation results showed that engine models that used different Cm2-Cms sets predicted similar combustion performance, when the spark timing, engine load, and engine speed were changed from the operating condition used to validate the CFD simulation. A dramatic shift was observed when engine speed was doubled, which suggested that the flame stretch coefficient, Cms, had a much larger influence at higher engine speeds compared to the flame development coefficient, Cm2. Therefore, the Cm2-Cms sets that predicted a higher turbulent flame under higher in-cylinder pressure and temperature increased the peak pressure and efficiency. This suggest that the choice of the Cm2-Cms will affect the G-equation-based simulation accuracy when engine speed increases from the one used to validate the model. As a result, for the less-experienced CFD user and in the absence of enough experimental data that would help retune the tuning parameters at various operating conditions, the purpose of a good G-equation-based 3D engine simulation is to guide and/or complement experimental investigations, not the other way around. Only a truly-predictive simulation that fully couples the turbulence/chemistry equations can help reduce the amount of experimental work.1
Original language | English |
---|---|
Journal | SAE Technical Papers |
Volume | 2018-April |
DOIs | |
State | Published - 2018 |
Event | 2018 SAE World Congress Experience, WCX 2018 - Detroit, United States Duration: Apr 10 2018 → Apr 12 2018 |
Funding
Notice: This manuscript has been authored by UT-Battelle, LLC, under contract DE-AC05-00OR22725 with the US Department of Energy (DOE). The US government retains and the publisher, by accepting the article for publication, acknowledges that the US government retains a nonexclusive, paid-up, irrevocable, worldwide license to publish or reproduce the published form of this manuscript, or allow others to do so, for US government purposes. DOE will provide public access to these results of federally sponsored research in accordance with the DOE Public Access Plan ( http://energy.gov/downloads/doe-public-access-plan ). The simulations were performed on the Super Computing System (Mountaineer) at WVU, which is funded in part by the National Science Foundation EPSCoR Research Infrastructure Improvement Cooperative Agreement #1003907, the state of West Virginia (WVEPSCoR via the Higher Education Policy Commission) and WVU. 1 This work was funded by the US Department of Energy’s Office of Vehicle Technologies under the guidance of the Advanced Combustion Engines and Systems program managed by Gurpreet Singh and Michael Weismiller. The CFD investigation and preparation of this manuscript was funded by West Virginia University and the Ralph E. Powe Junior Faculty Enhancement Award. The authors gratefully acknowledge the support of the Oak Ridge National Laboratory’s National Transportation Research Center and ANSYS®/Reaction Design® to this research.
Funders | Funder number |
---|---|
Ansys | |
National Transportation Research Center | |
US Department of Energy’s Office of Vehicle Technologies | |
WVEPSCoR | |
West Virginia | |
National Science Foundation | 1003907 |
U.S. Department of Energy | |
Oak Ridge National Laboratory | |
West Virginia University | |
West Virginia Higher Education Policy Commission |