CFD modelling of soot entrainment via thermophoretic deposition and crevice flow in a diesel engine
Introduction
The increasingly stringent regulations of diesel emissions in recent years have prompted concentrated efforts to improve engine designs and operations. However, certain modifications such as the use of exhaust gas recirculation (EGR) (Agarwal et al., 2011) and biodiesel as an alternative fuel in diesel engine (Park et al., 2012, Rakopoulos et al., 2011) have shown to have detrimental effects on the concentration of other pollutant species in the exhaust stream and the level of contaminant in engine oil. It is well known that high soot concentration in engine oil can clog filters and pyrolise into hard carbon deposit, which eventually lead to oil starvation and damage to the engine. Rounds (1977) proposed that wear occurs when the anti-wear additives which prevent metal-to-metal contact are adsorbed onto soot. Additionally, the viscosity of engine oil is raised, resulting in higher friction and invariably an increase in engine wear rate. The size of the soot particles also plays a significant role. Although nanosized soot particles are more dangerous in terms of health effects (Kittelson, 1997), an increase in soot diameter approaching the oil film thickness accelerates the engine wear rate (Sato et al., 1999).
During normal diesel engine operations, high soot concentrations are produced within the combustion chamber, and often exceed tenfold the exhaust soot concentrations. Within few hundred microns from the chamber wall, the local temperature is much lower and the soot particles in this region may escape oxidation (Eastwood, 2008). The existence of this temperature gradient gives rise to the thermophoretic process, where the particles move towards the region of lower temperature and deposit on the chamber wall. Thermophoresis is reported to be the major pathway of the soot deposition on the in-cylinder surfaces (Suhre & Foster, 1992). These soot particles are eventually scraped off by moving piston and entrain into the engine oil through the crevice during exhaust blowdown (Agarwal et al., 2011). Another pathway of soot entrainment into the engine oil is via crevice blowby, where the bulk mass of combustion product is transferred into the crankcase region through the crevice gap between the piston and the cylinder liner.
While extensive experimental work such as those reported by Shu et al. (2012) have been conducted to determine the key factors of combustion chamber deposit and its adverse effects, computational studies of soot deposition mechanism are employed to further understand this process. Most of these have been specifically focused on the thermophoretic effect. Dahlén (2002) conducted a CFD study of thermophoretic soot deposition in a diesel engine, where the predicted soot mass deposition data was fitted to the measurements of soot concentration in engine oil by adjusting the thermophoretic model constant. The predicted amount of soot deposition on the liner was found to agree well with the measured data, verifying the significance of the thermophoretic effect on soot entrainment process into engine oil. Thermophoretic deposition was also incorporated in a modelling study by Wiedenhoefer & Reitz (2003) to examine its effect on radiation in a heavy duty diesel engine. Here, radiative heat loss by soot in the near wall region was observed to be negligible. Ra & Reitz (2006) further investigated the engine soot deposition through the multidimensional modelling approach by introducing grids for complex geometry of the piston ring pack and submodels to represent the dynamics of crevice flow. The study concluded that crevice born hydrocarbon plays an important role in the formation of soot deposits.
In order to investigate the contribution of possible soot entrainment mechanisms, it is crucial to evaluate the effects of the operating strategies on spatial and temporal evolution of soot formed from the combustion process. In-cylinder soot formation is one of the most complicated processes occurring inside a diesel engine, and is strongly dependent on the evolution of the combusting spray jet and the transport processes. In-situ measurements to elucidate these processes may not be economically feasible, and as such, simulation study employing high fidelity CFD models are preferred for this purpose. The objective of this work is to computationally determine how injection parameters affects the soot entrainment process into the engine oil in a light-duty diesel engine, focussing specifically on the thermophoretic deposition on the liner and soot transport into the crevice region. The injection strategy appraised here includes single and split-main injection with different start of injection (SOI) timing, which have been developed by various researchers to extend the operating load range and improve emissions in diesel engine (Gan et al., 2011, Suh, 2011). By modifying the air fuel ratio, these injection strategies affect the formation of emission species as well as the soot particle size (Lapuerta et al., 2007), which subsequently impact the entrainment process into engine oil.
Section snippets
Engine geometries and operating conditions
In this study, the simulation is conducted based on a test engine with the specifications shown in Table 1. The engine is operated at a fixed engine speed of 1600 rev/min, while the brake mean effective pressure (BMEP) is maintained at 6.76 bar by varying the fuel mass delivered and hence the overall equivalence ratio. This simulation focuses only on the closed part of the engine cycle, from the intake valve closure (IVC) at −143 crank angle degree (CAD) after top dead centre (ATDC) to the
Numerical models
Numerical computation is conducted using ANSYS FLUENT 12, a commercial CFD software together with CHEMKIN-CFD as the chemistry solver. As shown in Fig. 1, the computational mesh represents 60° sector of the combustion chamber due to the symmetry imposed by the six equally spaced injector nozzle holes. The mesh is created with a cell size of 1.5 mm. Grid independent result was achieved with this setting and further refinement in the resolution was found to give insignificant improvement in the
Validation
Results of the simulated test cases are first validated against experimental data, which include the pressure trace, heat released rate (HRR) and tailpipe soot emission as shown in Fig. 2. Comparison between the experimental and simulated results shows that the over predictions in the ID of the main combustion event are maintained to within 1.5 CAD. The percentage error in the predicted peak pressure is less than 3.9%, with the offset in the peak pressure timing of less than 0.5 CAD. Similar
Results and discussions
The effects of different injection strategies on thermophoretic soot deposition on the cylinder liner and soot transport into the crevice region are presented here using appropriate illustrations of soot concentration distribution inside the combustion chamber. For ease of visualisation, the images of predicted soot concentration are shown in Fig. 3 as side view projections of the 3-D soot iso-surfaces, where the soot cloud layers are featured as semi-transparent. For each case, the soot images
Conclusion
A computational investigation on the effect of injection strategies on the soot entrainment into engine oil in a light-duty diesel engine is conducted. The total soot mass deposited on the liner is mainly dependent on the spatial and temporal evolution of the combustion soot cloud from the onset of the soot deposition process, while soot transport into the crevice takes place mainly at the EVO timing. In all the test cases, soot deposited on the liner is found to be the main contributor to the
Acknowledgement
The Faculty of Engineering at the University of Nottingham Malaysia Campus is acknowledged for the support towards this project. The Ministry of Science, Technology and Innovation (MOSTI) Malaysia is also acknowledged for the financial contribution towards the work.
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