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Effects of injection pressure and timing on low load Low Temperature Gasoline Combustion using LES

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... Combustion modes are principally categorized into spark ignition and compression ignition technologies. Compression ignition technologies encompass homogeneous charge compression ignition (HCCI) [44,64], partially premixed compression ignition (PPCI) [20,21,52], reactivity-controlled compression ignition (RCCI) [14,26], stratified charge compression ignition (SCCI) [13] and intelligent charge compression ignition (ICCI) [88,89]. Spark ignition technologies are further subdivided into thermal plasma ignition and non-thermal plasma ignition. ...
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Review Key Technologies to 50% Brake Thermal Efficiency for Gasoline Engine of Passenger Car Xinke Miao, Bingxin Xu, Jun Deng, and Liguang Li * School of Automotive Studies, Tongji University, Shanghai 201804, China * Correspondence: liguang@tongji.edu.cn Received: 13 August 2024; Revised: 6 December 2024; Accepted: 17 December 2024; Published: 20 January 2025 Abstract: As fuel consumption and emissions regulations become increasingly stringent, various advanced strategies have been proposed to achieve higher efficiency in internal combustion engines. This paper reviews the advancements in thermal efficiency of gasoline engines and analyzes the key technological methods to achieve over 50% brake thermal efficiency (BTE). The technological routes proposed for high-efficiency gasoline engine are primarily focused on high compression ratios and lean combustion combined with novel combustion technologies. Supporting technologies mainly include Atkinson/Miller cycles, intake boosting, exhaust gas re-circulation (EGR), water injection, thermal barrier coatings, friction reduction, structural optimization, and combustion diagnostics and control.
... Modeling ϵ SGS is extremely important for LES, which concludes a misunderstanding of the flow topology with artificial fluctuations by incorrect magnitude of C ϵ [56]. The Dynamic-Structure Large-Eddy Simulation (DS-LES) is used in this work, because this closure of the Leonard stresses has been shown to be highly accurate for mixing related flow physics compared with direct numerical simulation (DNS) data [57,58] and has a broad literature history of success for modeling flows with sharp temperature and density gradient [59,60,61,62,63]. Other LES subgrid closures are not evaluated in this work. ...
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Existing literature on ejectors, different researchers utilized different turbulence models by their choice, neither analyzing the physics of turbulence nor providing any sufficient optical diagnostics of the flow field. In this article, the physics captured by the Unsteady Reynolds Averaged Navier–Stokes (URANS) and Large Eddy Simulation (LES) are compared based on well-posed boundary conditions obtained experimentally from a carbon dioxide (CO2) vapor compression cycle with an error . The experimental results utilized for this study are at Reynold’s number (Re) 1.2e5 at the high-pressure inlet (motive flow) maintaining CO2 in subcritical state. The low-pressure inlet (suction flow) is maintained at Re = 9.8e4 with CO2 in vapor state, providing a pressure lift ratio of 1.2 at the diffuser outlet. Comparison of flow topologies with different URANS models reveals that only standard, Shear Stress Transport (SST) k-omega, and Reynold’s Stress Model-Shear Stress Gradient (RSM-SSG) are the suitable URANS models capturing a linearly increasing anisotropy tensor component with increasing strain in the flow. LES also predicted the similar physics. However, standard k-omega overpredicted the suction pressure beyond the acceptable uncertainty limits, which made it inapplicable. For the first time, a spatio-temporal representation of the flow topology with LES revealed the actual jet morphology of a CO2 ejector. Specifically, finger-like structures are key features to entrain more surrounding warm fluid into the colder dense core fluid at the cost of destabilizing and breaking up the jet by stretching the streamwise vortices and obstructing the increase in pressure-lift ratio.
... Compositional stratification is an integral part of new combustion technologies such as Low-Temperature Combustion (LTC), Homogeneous Charge Compression Ignition (HCCI), Moderate and Intense Low-oxygen Dilution (MILD), etc. The compositional stratification is generally achieved in engines using direct injection inside the combustion chamber (Agarwal et al. 2023;Tan et al. 2016;O'Donnell et al. 2023) or by dilution of the fuel-air mixture (Telli et al. 2022;Fooladgar and Chan 2017;Zhao et al. 2019). With stratification, stoichiometric or slightly rich mixtures can be used near the ignition source, and ultra-lean mixtures can be used near the chamber walls. ...
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Gasoline direct injection engines can provide higher thermal efficiency and lower emissions than that for engines using conventional combustion techniques. Compositional stratification inside the combustion chamber opens possibilities for ultra-lean and low-temperature combustion. To explore this further, 2D direct numerical simulation (DNS) has been performed to investigate the propagation of syngas flame in an equivalence ratio (ϕ) stratified medium. Several aspects of flame propagation, such as effect of integral scale of mixing (lϕ) on the non-monotonic behavior of flame propagation, contribution of each chemical reaction to heat release rate (HRR), and the effect of differential diffusion were analyzed using DNS-data. A spherically expanding flame has been initiated with a hotspot at the center of the square domain of size 2.4 × 2.4 cm². The variations in the degree of stratification were simulated varying lϕ and fluctuations ϕ for initial mixture distribution. Further this DNS-data has been used to analyze effects of stratification on flame displacement speed (Sd) and its components, viz. reaction rate (Sr), normal diffusion (Sn), tangential (St), and inhomogeneity (Sz). The results reveal that stratification-induced variations in thermal diffusivity resulted in thermal runaways. These thermal runaways influence the extent of burning for simulated cases. The increase in degree of stratification resulted in flame preferably propagating towards leaner ϕ, causing reduction in components of Sd. The preferential propagation of flame also resulted in shifting of peak reaction rate for fuel species (c*) to a higher reaction progress variable (c). This shifting of c*, lead to a reduction in the HRR contribution of reactions that attain their peak near the production zone of H and OH species. For unity Le simulations, Sn was observed to be reduced drastically compared to cases with differential diffusion, resulting in an overall reduction in Sd.
... Compositional stratification is an integral part of new combustion technologies such as Low-Temperature Combustion (LTC), Homogeneous Charge Compression Ignition (HCCI), Moderate and Intense Low-oxygen Dilution (MILD), etc. The compositional stratification is generally achieved in engines using direct injection inside the combustion chamber [4][5][6] or by dilution of the fuel-air mixture [7][8][9]. With stratification, stoichiometric or slightly rich mixtures can be used near the ignition source, and ultra-lean mixtures can be used near the chamber walls. ...
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Gasoline direct injection (GDI) engines can provide higher thermal efficiency and lower emissions compared to conventional combustion techniques. The direct charge injection near the ignition source forms compositional stratification inside the combustion chamber. Compositional stratification inside the combustion chamber opens possibilities for ultra-lean and low-temperature combustion. In this paper, a 2D direct numerical simulation (DNS) has been performed to investigate the propagation of syngas flame in an equivalence ratio stratified medium. A spherically expanding flame has been initiated with a hotspot at the center of the domain. An open-source PENCIL code [Babkovskaia, 2011] is used to analyse the effect of stratification by simulating cases with varying integral scales of mixing ( l ϕ ) and fluctuations of equivalence ratio ( ϕ´ ). Effects of differential diffusion of species on flame propagation have also been examined by comparing results with cases with unity Lewis number ( Le =1). The results show that with an increase in l ϕ , flame propagation shows a non-monotonic behavior. With an increase in l ϕ , the flame speed and extent of burning increase first and then decrease. With an increase in ϕ´, the flame speed and extent of burning decreased consistently. The peak reaction rate of fuel species is also observed to be shifted to a higher reaction progress variable ( c ) with increased stratification. The effect of stratification and differential diffusion has been analysed for four identified components of flame displacement speed ( S d ) viz. reaction ( S r ), normal diffusion ( S n ), tangential ( S t ), and inhomogeneity ( S z ). S r and S n are observed to be major contributors to S d . The magnitude of S r shows reductions with an increase in stratification. In comparison, S n does not show significant change with increased stratification. The variation of the contribution of chemical reactions to heat release rate with stratification is also analysed in this study. The results show that shifting of peak reaction rate of fuel species to higher c values results in variation in heat release rate contribution for chemical reactions.
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Advanced combustion concepts, like homogeneous charge compression ignition, are limited by their narrow operating range, which stems from a lack of control over the heat release process. This study explores a new advanced combustion mode, called thermally stratified compression ignition, which uses a direct water injection event to control the heat release process in low-temperature combustion. A three-dimensional computational fluid dynamics model coupled with detailed chemical kinetics is used to better understand the effects of direct water injection on thermal stratification in the cylinder and the resulting heat release process. Previous results showed that increasing the injection pressure results in a significantly broader temperature distribution due to increased evaporative cooling. In this way, direct water injection can control low-temperature combustion heat release and extend significantly the operable load range. In this study, simulations were performed over a range of start of injection timings in order to determine its effect on thermal stratification and heat release. The results show that for both low and high injection pressures advancing the start of water injection results in increased thermal stratification and reduced peak pressure and heat release rate for injections occurring after −60 °CAD. Before −60 °CAD, advancing the water injection has a varied effect on thermal stratification and heat release depending on the injection pressure and mass of the injected water.
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Thermal stratification of the unburned charge prior to ignition plays a significant role in governing the heat release rates in a homogeneous charge compression ignition (HCCI) engine. A deep understanding of the conditions affecting thermal stratification is necessary for actively managing HCCI burn rates and expanding its operating range. To that end, a single-cylinder gasoline-fueled HCCI engine was used to characterize the relationship between key operating conditions, such as intake temperature, residual gas fraction, air-to-fuel ratio, and swirl, and thermal stratification. The recently developed Thermal Stratification Analysis was applied to calculate the unburned temperature distribution prior to ignition from heat release.
Article
This work explores the potential of partial fuel stratification to smooth HCCI heat-release rates at high load. A combination of engine experiments and multi-zone chemical-kinetics modeling was used for this. The term "partial" is introduced to emphasize that care is taken to supply fuel to all parts of the in-cylinder charge, which is essential for reaching high power output. It was found that partial fuel stratification offers good potential to achieve a staged combustion event with reduced pressure-rise rates. Therefore, partial fuel stratification has the potential to increase the high-load limits for HCCI/SCCI operation. However, for the technique to be effective the crank-angle phasing of the "hot" ignition has to be sensitive to the local φ. Sufficient sensitivity was observed only for fuel blends that exhibit low-temperature heat release (like diesel fuel). In contrast, for a single-stage ignition fuel (like typical gasoline) the timing of the hot ignition is relatively insensitive to the local φ, and this renders partial fuel stratification ineffective for creating a staged combustion event. The effects of partial fuel stratification were demonstrated experimentally for PRF80 and PRF83 fuels using a hollow-cone DI injector and two fuel-injection pulses. Suitable fuel stratification was created by injecting the main portion of the fuel during the intake stroke, and the remainder during the compression stroke. This smoothed the heat-release and lowered the pressure-rise rate significantly compared to fully-premixed fueling. For naturally aspirated operation with CA50 at 371°CA, partial fuel stratification allowed IMEP g to be increased from 537 to 597 kPa while maintaining acceptable ringing intensity (PRRmax < 8 bar/°CA) and NOx emissions below US 2010 standards. However, partial fuel stratification must be implemented carefully since too much stratification can quickly lead to unacceptable NOx emissions.
Article
When oxygen reacts with pyro graphite at high flow rates and at pressures of about 0.2 atm, the reaction rate increases steeply with temperature from 1050°C to 1700°C; above this temperature the rate ceases to rise and the reaction curve becomes nearly horizontal. Since much faster rates of reaction are observed with other forms of carbon under otherwise identical reaction conditions, the pyro graphite rates must be genuine chemical rates not substantially influenced by gas phase mass transfer. In the past the reactions of oxygen at very low pressures with carbon filaments have shown that the reaction curve under these conditions reaches a maximum at a temperature of about 1100°C, which is 600°C less than the temperature at which the maximum rate with pyro graphite at a pressure of 0.2 atm was observed. The theory of Blyholder, Binford and Eyring, slightly modified, is shown to account satisfactorily for this difference between the low and high pressure results. The reactions of reactor quality graphite with oxygen have also been studied. The reaction curves reach a maximum at about 1600°C in a manner very similar to those of pyro graphite, and the rate then falls appreciably between 1600°C and 2000°C. The rates in this case are considerably higher than with pyro graphite, and they are certainly partly mass-transfer controlled: but the similarity in shape with the pyro graphite results suggests that, although the absolute values of the rates may be in need of considerable correction for mass transfer, the curves for reactor graphite are in broad outline of a shape determined by chemical factors.
Article
Unlabelled: The U.S. Environmental Protection Agency (EPA) established strict regulations for highway diesel engine exhaust emissions of particulate matter (PM) and nitrogen oxides (NOx) to aid in meeting the National Ambient Air Quality Standards. The emission standards were phased in with stringent standards for 2007 model year (MY) heavy-duty engines (HDEs), and even more stringent NOX standards for 2010 and later model years. The Health Effects Institute, in cooperation with the Coordinating Research Council, funded by government and the private sector, designed and conducted a research program, the Advanced Collaborative Emission Study (ACES), with multiple objectives, including detailed characterization of the emissions from both 2007- and 2010-compliant engines. The results from emission testing of 2007-compliant engines have already been reported in a previous publication. This paper reports the emissions testing results for three heavy-duty 2010-compliant engines intended for on-highway use. These engines were equipped with an exhaust diesel oxidation catalyst (DOC), high-efficiency catalyzed diesel particle filter (DPF), urea-based selective catalytic reduction catalyst (SCR), and ammonia slip catalyst (AMOX), and were fueled with ultra-low-sulfur diesel fuel (~6.5 ppm sulfur). Average regulated and unregulated emissions of more than 780 chemical species were characterized in engine exhaust under transient engine operation using the Federal Test Procedure cycle and a 16-hr duty cycle representing a wide dynamic range of real-world engine operation. The 2010 engines' regulated emissions of PM, NOX, nonmethane hydrocarbons, and carbon monoxide were all well below the EPA 2010 emission standards. Moreover, the unregulated emissions of polycyclic aromatic hydrocarbons (PAHs), nitroPAHs, hopanes and steranes, alcohols and organic acids, alkanes, carbonyls, dioxins and furans, inorganic ions, metals and elements, elemental carbon, and particle number were substantially (90 to >99%) lower than pre-2007-technology engine emissions, and also substantially (46 to >99%) lower than the 2007-technology engine emissions characterized in the previous study. Implications: Heavy-duty on-highway diesel engines equipped with DOC/DPF/SCR/AMOX and fueled with ultra-low-sulfur diesel fuel produced lower emissions than the stringent 2010 emission standards established by the U.S. Environmental Protection Agency. They also resulted in significant reductions in a wide range of unregulated toxic emission compounds relative to older technology engines. The increased use of newer technology (2010+) diesel engines in the on-highway sector and the adaptation of such technology by other sectors such as nonroad, displacing older, higher emissions engines, will have a positive impact on ambient levels of PM, NOx, and volatile organic compounds, in addition to many other toxic compounds.
Article
This study investigates the potential of partial fuel stratification for reducing the knocking propensity of intake-boosted HCCI engines operating on conventional gasoline. Although intake boosting can substantially increase the high-load capability of HCCI, these engines would be more production-viable if the knock/stability load limit could be extended to allow higher loads at a given boost and/or to provide even higher thermal efficiencies. A technique termed partial fuel stratification (PFS) has recently been shown to greatly reduce the combustion-induced pressure-rise rate (PRR), and therefore the knocking propensity of naturally aspirated HCCI, when the engine is fueled with a φ-sensitive, two-stage-ignition fuel. The current work explores the potential of applying PFS to boosted HCCI operation using conventional gasoline, which does not typically show two-stage ignition. Experiments were conducted in a single-cylinder HCCI research engine (0.98 liters) at 1200 rpm. The engine was equipped with a compression-ratio 14 piston, and combustion phasing was controlled by EGR addition. PFS is produced by premixing the majority of the fuel and then directly injecting the remainder (up to about 20%) in the latter part of the compression stroke. For PFS to be effective, the fuel's autoignition chemistry must vary with the local equivalence ratio (φ) to produce a staged combustion event. Accordingly, tests were conducted to determine the φ-sensitivity of gasoline. They show that at naturally aspirated conditions (P in = 1 bar), gasoline is not φ-sensitive, and PFS is not effective for reducing the PRR. However, with sufficient intake boost (e.g. P in = 2 bar), gasoline is found to become highly φ-sensitive, and PFS very effectively reduces the PRR. Varying the amount of PFS, by adjusting either the timing or amount of DI fuel, allows control of the PRR reduction. Applying PFS to high loads at P in = 2 bar substantially shifts the knock/stability limit and increases the maximum IMEP g from 11.7 (premixed) to 13.0 bar (PFS). Maximum load improvements with PFS are also seen for other intake pressures ranging from 1.6 to 2.4 bar. Finally, because it allows more advanced combustion phasing without knock, PFS is also effective for increasing the thermal efficiency of boosted HCCI over a range of loads for each P in, yielding typical fuel economy improvements of 2 - 2.5%. Overall, PFS has a strong potential for improving gasoline-fueled boosted HCCI operation.
Conference Paper
Recent measurements by Siebers et al. have shown that the flame of a high pressure Diesel spray stabilizes under quiescent conditions at a location downstream of the fuel injector. The effects of various ambient and injection parameters on the flame “lift-off” length have been investigated under typical Diesel conditions in a constant-volume combustion vessel. In the present study, the experiments of Siebers et al. have been modeled using a modified version of the KIVA-3V engine simulation code. Fuel injection and spray breakup are modeled using the KH-RT model that accounts for liquid surface instabilities due to the Kelvin-Helmholtz and Rayleigh-Taylor mechanisms. Combustion is simulated using Convergent Thinking's recently developed detailed transient chemistry solver (SAGE) that allows for any number of chemical species and reactions to be modeled. While detailed chemistry is believed to be an accurate methodology for modeling Diesel combustion, in the past the extensive run times rendered it impractical. To expedite the calculations, SAGE has been implemented into KIVA using the Message-Passing Interface (MPI). This implementation allows for the chemical reactions to be simulated in parallel on multiple CPUs. An n-heptane mechanism was used to model Diesel fuel ignition and combustion. The improved KIVA-3V code was used to simulate the spray-bomb cases over a wide range of injection pressures, nozzle hole sizes, ambient temperatures, and ambient densities. In general, excellent agreement was obtained between the measurements and simulation results for liquid length and flame lift-off length. To further validate the chemical kinetics model, simulations of a heavy-duty direct injection Diesel engine were conducted. The results indicate that the detailed chemistry model is able to accurately predict ignition delay and cylinder-averaged pressure for a range of start of injection timings.
Article
Engine experiments and multi-dimensional modeling were used to explore Reactivity Controlled Compression Ignition (RCCI) to realize highly-efficient combustion with near zero levels of NOx and PM. In-cylinder fuel blending using port-fuel-injection of a low reactivity fuel and optimized direct-injection of higher reactivity fuels was used to control combustion phasing and duration. In addition to injection and operating parameters, the study explored the effect of fuel properties by considering both gasoline-diesel dual-fuel operation, ethanol (E85)-diesel dual fuel operation, and a single fuel gasoline-gasoline+DTBP (di-tert butyl peroxide cetane improver). Remarkably, high gross indicated thermal efficiencies were achieved, reaching 59%, 56%, and 57% for E85-diesel, gasoline-diesel, and gasoline-gasoline+DTBP respectively. Using conditions based on CFD simulations, engine experiments were performed using a heavy-duty test engine and the modeling was further used to explain the experimentally observed results. The experiments confirmed that by optimizing the fuel reactivity based on the specific operating conditions, combustion phasing can be optimized in order to minimize fuel consumption. Additionally, it was found that highly efficient operation (greater than 50% indicated thermal efficiency) could be achieved with all three fuel blending strategies over a wide range of loads. This study showed that, compared to gasoline-diesel, significantly higher quantities of diesel fuel were required to maintain optimal combustion phasing with the E85-diesel fuel blends. This result is due to a combination of the lower reactivity and higher enthalpy of vaporization of ethanol (compared to gasoline) and combustion chemistry effects of ethanol diesel blends. Secondly, the single fuel gasoline-gasoline+DTBP yielded near identical emissions and ISFC results to gasoline-diesel operation. Although the emissions and ISFC of all three strategies were similar, the low temperature heat release (LTHR) were different with all three fuels, and the high temperature heat release (HTHR) was different with E85-diesel blends. Fuel chemistry effects for all three fuels were investigated and their effect on the reactivity gradient was found to be responsible for the combustion differences.
Article
Reactivity Controlled Compression Ignition combustion (RCCI) has been demonstrated at mid to high loads [1, 2, 3, 4, 5, 6] as a method to operate an internal combustion engine that produces low NOx and low PM emissions with high thermal efficiency. The current study investigates RCCI engine operation at loads of 2 and 4.5 bar gross IMEP at engine speeds between 800 and 1700 rev/min. This load range was selected to cover the range from the previous work of 6 bar gIMEP down to an off-idle load at 2 bar. The fueling strategy for the low load investigation consisted of in-cylinder fuel blending using port-fuel-injection of gasoline and early cycle, direct-injection of either diesel fuel or gasoline doped with 3.5% by volume 2-EHN (2-ethylhexyl nitrate). At these loads, engine operating conditions such as inlet air temperature, port fuel percentage, and engine speed were varied to investigate their effect on combustion. Results show that at the 4.5 bar gIMEP operating condition it was possible to maintain 54% gross indicated thermal efficiency with NOx and PM emissions below US EPA 2010 limits. The results also show that it is possible to operate at a near idle load of 2 bar gross IMEP load with a gross indicated thermal efficiency of 49% at 1300 rev/min and 44% at 800 rev/min.
Article
A reduced PRF mechanism was proposed for combustion simulations of PRF and diesel/gasoline fuels based on the latest LLNL mechanism. The reduced PRF mechanism consists of 73 species and 296 reactions. The major reaction pathways of the detailed mechanism were mostly retained in the reduced mechanism, which ensures its predictive capability, the ability to be extended to other fuels, and the high computational efficiency of the reduced mechanism. The important reaction pathways and reactions in the reduced mechanism are identified and discussed. Furthermore, the reaction rates of two reactions, HO2 + OH = HO2 + O2 and HO2 + HO2 = H2O2 + O2, in the hydrogen submechanism are discussed and updated. The reduced mechanism was validated with measured ignition delays, laminar flame speeds, premixed flame species concentrations, jet stirred reactor and shock tube species profiles, and PRF fuel HCCI and PPCI combustion and diesel/gasoline direct injection spray combustion data. The reduced mechanism predicts well the ignition timings, flame speeds, and important species concentrations under various validation conditions and shows reliable performance under different engine validation conditions. The overall results suggest that the current mechanism can provide reliable predictions for PRF and diesel/gasoline combustion CFD simulations.
Article
Fuel stratification is a potential strategy for reducing the maximum pressure rise rate in HCCI engines. Simulations of Partial Fuel Stratification (PFS) have been performed using CONVERGE with a 96-species reduced mechanism for a 4-component gasoline surrogate. Comparison is made to experimental data from the Sandia HCCI engine at a compression ratio 14:1 at intake pressures of 1 bar and 2 bar. Analysis of the heat release and temperature in the different equivalence ratio (φ) regions reveals that sequential auto-ignition of the stratified charge occurs in order of increasing φ for 1 bar intake pressure but in order of decreasing φ for 2 bar intake pressure. Increased low- and intermediate-temperature heat release at 2 bar intake pressure compensates for decreased temperatures in higher-φ regions due to evaporative cooling from the liquid fuel spray and decreased compression heating from lower values of the ratio of specific heats. At 1 bar intake pressure, the premixed portion of the charge auto-ignites before the highest-φ regions and the sequential auto-ignition occurs too fast for useful reduction of the maximum pressure rise rate compared to HCCI. Conversely, at 2 bar intake pressure, the premixed portion of the charge auto-ignites last, after the higher-φ regions. More importantly, the sequential auto-ignition occurs over a longer time period than at 1 bar intake pressure such that a sizable reduction in the maximum pressure rise rate compared to HCCI can be achieved.
Article
Recent direct numerical simulations of constant density isobaric turbulent flame-wall interaction have lead to the development of a wall model that can easily be implemented in turbulent combustion models used in conventional CFD codes (as e.g. flamelet models). An essential point of this model is the estimation of the mean heat loss of the turbulent flame brush to the cold combustion chamber walls, emphasizing the need for an accurate description of the boundary conditions on solid walls in terms of wall heat transfer and turbulence. With regard to mesh size and computing time, most industrial CFD codes use high-Reynolds number k - ε turbulence models in conjunction with a law-of-the-wall to describe near wall flow conditions. One important assumption for the validity of the law-of-the-wall is that the near wall flow is isothermal, the fluid properties in this region thus being regarded as constant. This assumption is obviously erronous in flows combining hot gases (generated by combustion and/or compression) with cold walls, as in IC engines. We present a formulation of the law-of-the-wall that is equivalent to the classical one when the wall flow is isothermal and takes into account effects of variable fluid properties for non-isothermal conditions. A modification of the above cited turbulent combustion model is proposed to describe non-isobaric flame-wall interaction in SI engines. Both models are implemented in the KIVA-II code and are first validated on a simple axisymmetric pancake SI engine. The new models are shown to more accurately reproduce experimental local wall heat fluxes and pressure/time histories than the original ones. Finally, computations of intake and combustion in a 4-valve SI engine geometry show the ability of the new models to reproduce global engine characteristics quite satisfactorily over a range of operating parameters.
Article
Chemiluminescence experiments were conducted in a single-cylinder HCCI engine to provide a comprehensive understanding of the effects of temperature and mixture stratification on HCCI combustion. Chemiluminescence spectrum and CFD coupled kinetics models were used to analyze the combustion mechanism under different stratification. Results indicated that the different port injection strategies resulted in different mixture stratifications, thus affected the auto-ignition timing and combustion processes. Under higher intake temperature conditions, injection strategies had less effect on the combustion processes due to improved evaporating and mixing. Some of the chemical kinetic reactions were “frozen” due to the low local temperature in the whole combustion process for lower coolant temperature. Increased temperature stratification was undesirable to low load conditions because more quenching would occur at the cooler regions in the cylinder. It can be concluded that the port injection timing, turbulence generated by higher engine speed, different intake and coolant temperatures can affect combustion processes in HCCI engines. The essence of these factors was their impact on the temperature distribution in the cylinder during combustion. Larger local temperature stratification can reduce the pressure rise rate through smoothing the reaction rates and extend the operating range in HCCI engines.
Article
Homogeneous charge compression ignition (HCCI) combustion with fully premixed charge is severely limited at high-load operation due to the rapid pressure-rise rates (PRR) which can lead to engine knock and potential engine damage. Recent studies have shown that two-stage ignition fuels possess a significant potential to reduce the combustion heat release rate, thus enabling higher load without knock.
Article
In this study, a one-equation LES sub-grid model from Menon, et al. (5) is used in simulating the diesel combustion process. In addition, based on the one- equation methodology of Menon et al., a new one- equation LES scalar transport model is formulated. These models allow for the turbulent transfer coefficients for both momentum and scalar flux to be determined independent of each other. The turbulent viscosity, t µ , is determined as a function of the sub-grid kinetic energy, which is in turn determined from the one- equation model. The formulation for the scalar transfer coefficient, s µ , is similar to that of the turbulent viscosity, yet is made to be consistent with scalar transport. Results for the LES momentum transfer are compared to experimental data of a backward facing step. This model, in conjunction with the LES scalar flux model, is verified by comparing with experimental data for a non- reacting turbulent jet. Finally, these models are used with a Probability Density Function (PDF) combustion model to model the diesel combustion process. The presented results indicate that that LES is a viable option for simulating the turbulent reacting processes that occur within the diesel environment.
Article
This work concerns one of the major issues restricting the application of homogeneous charge compression-ignition (HCCI) engines, overly rapid combustion at high-load conditions, which can lead to engine knock and potential engine damage. To overcome this problem, partial fuel stratification was used, where most fuel was premixed with intake air and the rest of the fuel was directly injected during the compression stroke. To be effective, this technique depends critically on the fuel autoignition chemistry. PRF73, a mixture of 73vol% isooctane and 27vol% n-heptane that exhibits two-stage ignition under these conditions, successfully enabled control of the combustion heat-release rate with properly adjusted injection parameters. More than a 70% reduction in the maximum pressure-rise rate (PRRmax) was achieved, compared to the fully premixed case at the same combustion phasing. Meanwhile, combustion remained stable, efficient, and clean. In particular, NOx emissions were kept well below the US-2010 limits. On the other hand, isooctane, which exhibits single-stage ignition under the present conditions, responded much differently to partial fuel stratification. Instead of reducing PRRmax, isooctane partial stratification increased PRRmax and drastically raised NOx emissions and combustion instability. Such differences between single- and two-stage fuels result from the different response of their autoignition rates to the variations in equivalence ratio produced by partial fuel stratification, termed ϕ-sensitivity.
Article
While engineering applications of the large eddy simulation (LES) technique are becoming a common reality in many branches of engineering and science, its application to engine flows has lagged behind due to the relatively more complex nature of both the flow and the geometry relevant to in-cylinder flows. In this paper a review of the limited number of LES applications to engine flows is given, and most significant results from these studies are presented. Also, the LES formulation appropriate for engine applications is briefly described, along with the main characteristics of in-cylinder flows. As expected, engine applications of LES are not of the so-called ‘high-fidelity’ type, but rather they employ formally second-order accurate numerical schemes in conjunction with finite volume formulation. The subgrid scale (SGS) models used are also kept as simple as possible, mostly using a variant of the Smagorinsky model. Nevertheless, this review reveals that even with relatively coarse grids, LES captures much more interesting features of in-cylinder flows, such as the large coherent vortical flow structures developed during the intake stroke. In the opinion of the present authors, a low-resolution LES provides a better solution than RANS (Reynolds averaged Navier-Stokes) with moderate grid resolution because the important features of flow dynamics cannot be reproduced in RANS due to the high level of non-physical diffusion. Of course, some overheads in computational costs must be paid for this benefit obtained from LES.
Article
In the light of rapidly increasing applications of large-eddy-simulations (LES) it is deemed necessary to impose some quality assessment measures for such studies. The validation of LES is difficult because of the fact that both the sub-grid scale (sgs) model contribution and numerical discretization errors are functions of the grid resolution. In this study various index of quality measures, here and after referred to as LES_IQ, are proposed and applied to some case studies. The recommended LES_IQ is based on the concept of Richardson’s extrapolation. It is postulated that in practical applications of LES numerical dissipation will always be a significant part of the overall dissipation and it must be accounted for in any assessment of the quality of LES results. It is further suggested that an LES_IQ of 75% to 85% can be considered adequate for most engineering applications that typically occur at high Reynolds numbers; LES-IQ greater than 90% can be classified as DNS.
Conference Paper
A multi-dimensional model was used to calculate interactions between spray drops and gas motions close to the nozzle in dense high-pressure sprays. The model also accounts for the phenomena of drop breakup, drop collision and coalescence, and the effect of drops on the gas turbulence. The calculations used a new method to describe atomization (a boundary condition in current spray codes). The method assumes that atomization and drop breakup are indistinguishable processes within the dense spray near the nozzle exit. Accordingly, atomization is prescribed by injecting drops ('blobs') that have a size equal to the nozzle exit diameter.