"The hazard associated with dust deflagrations has increased over the last decade industries that manufacture, transport, process, or use combustible dusts. Identification of the controlling parameters of dust deflagration mechanisms is crucial to our understanding of the problem. The objective of this study is to develop an experimental platform, called the Hybrid Flame Analyzer (HFA), capable of measuring the laminar and turbulent burning velocity of gas, dust, and hybrid (gas and dust) air premixed flames as a function of properties specific to the reactants such as dust-particle size and concentration. In this work the HFA is used to analyze a particle-gas-air premixed system composed of coal dust particles (75-90 µm and 106-120 µm) in a premixed CH4-air ( = 0.8, 1.0 and 1.2) flame. This work ultimately aims to improve the knowledge on fundamental aspects of dust flames which is essential for the development of mathematical models. This study is the first of its kind where multiple different parameters that govern flame propagation (initial particle radius, particle concentration, gas phase equivalence ratio, turbulent intensity, and integral length scale) are systematically analyzed in a spatially uniform cloud of volatile particles forming a stationary flame. The experiments show that the turbulent burning velocity is more than two-times larger than the laminar counter-part for each and every case studied. It is observed that smaller particles and larger concentrations (> 50 g/m3) tend to enhance the turbulent burning velocity significantly compared to larger particle sizes and lower concentration ranges. The experimental data is used to develop a correlation similar to turbulent gas flames to facilitate modeling of the complex behavior. "

No description available.

Considering the importance of combustion characteristics in combustion applications including spark ignition engines and gas turbines, both laminar and turbulent burning velocities were measured for gasoline related fuels. The first part of the present work focused on the measurements of laminar burning velocities of Fuels for Advanced Combustion Engines (FACE) gasolines and their surrogates using a spherical constant volume combustion chamber (CVCC) that can provide high-pressure high-temperature (HPHT) combustion mode up to 0.6 MPa, 395 K, and the equivalence ratios ranging 0.7-1.6. The data reduction was based on the linear and nonlinear extrapolation models considering flame stretch effect. The effect of flame instability was investigated based on critical Peclet and Karlovitz, and Markstein numbers. The sensitivity of the laminar burning velocity of the aforementioned fuels to various fuel additives being knows as octane boosters and gasoline extenders including alcohols, olfins, and SuperButol was investigated. This part of the study was further extended by examining exhaust gas re-circulation effect. Tertiary mixtures of toluene primary reference fuel (TPRF) were shown to successfully emulate the laminar burning characteristics of FACE gasolines associated with different RONs under various experimental conditions. A noticeable enhancement of laminar burning velocities was observed for blends with high ethanol content (vol ≥ 45 %). However, such enhancement effect diminished as the pressure increased. The reduction of laminar burning velocity cause by real EGR showed insensitivity to the variation of the equivalence ratio. The second part focused on turbulent burning velocities of FACE-C gasoline and its surrogates subjected to a wide range of turbulence intensities measured in a fan-stirred CVCC dedicated to turbulent combustion up to initial pressure of 1.0 MP. A Mie scattering imaging technique was applied revealing the mutual flame-turbulence interaction. Furthermore, considerable efforts were made towards designing and commissioning a new optically-accessible fan-stirred HPHT combustion vessel. A time-resolved stereoscopic particle image velocimetry (TR-PIV) technique was applied for the characterization of turbulent flow revealing homogeneous-isotropic turbulence in the central region to be utilized successfully for turbulent burning velocity measurement. Turbulent burning velocities were measured for FACE-C and TPRF surrogate fuels along with the effect of ethanol addition for a wide range of initial pressure and turbulent intensity. FACE-C gasoline was found to be more sensitive to both primarily the primary contribution of turbulence intensification and secondarily from pressure in enhancing its turbulent burning velocity. Several correlations were validated revealing a satisfactory scaling with turbulence and thermodynamic parameters. The final part focused on the turbulent burning characteristics of piloted lean methane-air jet flames subjected to a wide range of turbulence intensity by adopting TR-SPIV and OH-planar laser-induced florescence (OH-PLIF) techniques. Both of the flame front thickness and volume increased reasonably linearly as normalized turbulence intensity, u^'/ S_L^0, increased. As u^'/ S_L^0 increased, the flame front exhibited more fractalized structure and occasionally localized extinction (intermittency). Probability density functions of flame curvature exhibited a Gaussian like distribution at all u^'/ S_L^0. Two-dimensional flame surface density (2D-FSD) decreased for low and moderate u^'/ S_L^0, while it increased for high u^'/ S_L^0Turbulent burning velocity was estimated using flame area and fractal dimension methods showing a satisfactory agreement with the flamelet models by Peters and Zimont. Mean stretch factor was estimated and found to increase linearly as u^'/ S_L^0increased. Conditioned velocity statistics were obtained revealing the mutual flame-turbulence interaction.

Turbulent premixed propane/air and methane/air flames were studied using planar Rayleigh scattering and particle image velocimetry on a stabilized Bunsen type burner. The fuel-air equivalence ratio was varied from Φ=0.7 to 1.0 for propane flames, and from Φ=0.6 to 1.0 for methane flames. The non-dimensional turbulence intensity, u'/SL (ratio of fluctuation velocity to laminar burning velocity), covered the range from 3 to 24, equivalent to conditions of corrugated flamelets and thin reaction zones regimes. Temperature gradients decreased with the increasing u'/SL and levelled off beyond u'/SL > 10 for both propane and methane flames. Flame front thickness increased slightly as u'/SL increased for both mixtures, although the thickness increase was more noticeable for propane flames, which meant the thermal flame front structure was being thickened. A zone of higher temperature was observed on the average temperature profile in the preheat zone of the flame front as well as some instantaneous temperature profiles at the highest u'/SL. Curvature probability density functions were similar to the Gaussian distribution at all u'/SL for both mixtures and for all the flame sections. The mean curvature values decreased as a function of u'/SL and approached zero. Flame front thickness was smaller when evaluated at flame front locations with zero curvature than that with curvature. Temperature gradients and FSD were larger when the flame curvature was zero. The combined thickness and FSD data suggest that the curvature effect is more dominant than that of the stretch by turbulent eddies during flame propagation. Integrated flame surface density for both propane and methane flames exhibited no dependance on u'/SL regardless of the FSD method used for evaluation. This observation implies that flame surface area may not be the dominant factor in increasing the turbulent burning velocity and the flamelet assumption may not be valid under the conditions studied. Dκ term, the product of diffusivity evaluated at conditions studied and the flame front curvature, was a magnitude smaller than or the same magnitude as the laminar burning velocity.

Turbulent premixed propane/air and methane/air flames were studied using planar Rayleigh scattering and particle image velocimetry on a stabilized Bunsen type burner. The fuel-air equivalence ratio was varied from Φ=0.7 to 1.0 for propane flames, and from Φ=0.6 to 1.0 for methane flames. The non-dimensional turbulence intensity, u'/SL (ratio of fluctuation velocity to laminar burning velocity), covered the range from 3 to 24, equivalent to conditions of corrugated flamelets and thin reaction zones regimes. Temperature gradients decreased with the increasing u'/SL and levelled off beyond u'/SL > 10 for both propane and methane flames. Flame front thickness increased slightly as u'/SL increased for both mixtures, although the thickness increase was more noticeable for propane flames, which meant the thermal flame front structure was being thickened. A zone of higher temperature was observed on the average temperature profile in the preheat zone of the flame front as well as some instantaneous temperature profiles at the highest u'/SL. Curvature probability density functions were similar to the Gaussian distribution at all u'/SL for both mixtures and for all the flame sections. The mean curvature values decreased as a function of u'/SL and approached zero. Flame front thickness was smaller when evaluated at flame front locations with zero curvature than that with curvature. Temperature gradients and FSD were larger when the flame curvature was zero. The combined thickness and FSD data suggest that the curvature effect is more dominant than that of the stretch by turbulent eddies during flame propagation. Integrated flame surface density for both propane and methane flames exhibited no dependance on u'/SL regardless of the FSD method used for evaluation. This observation implies that flame surface area may not be the dominant factor in increasing the turbulent burning velocity and the flamelet assumption may not be valid under the conditions studied. Dκ term, the product of diffusivity evaluated at conditions studied and the flame front curvature, was a magnitude smaller than or the same magnitude as the laminar burning velocity.

Une des solutions pour diminuer les émissions polluantes émises par un moteur à combustion interne est de réinjecter une partie des gaz d’échappement (Exhaust Gas Recirculation, EGR) à l'admission. Cependant, dans le cas d’une dilution du mélange air-carburant trop importante, la combustion est plus instable voire ne pas s’entretenir. L’ajout d’une faible quantité d’hydrogène a le potentiel de contrer cet effet négatif de forte dilution. C’est dans ce contexte que ce travail de thèse est basé sur une étude détaillée des effets combinés de l’ajout de l’hydrogène et de la dilution dans un moteur à allumage commandé alimenté par du méthane ou de l’iso-octane. Dans la première partie de ce travail, le potentiel de l’ajout de l’hydrogène combiné à la dilution, en termes d’émissions polluantes et de rendement global du moteur, est montré. Dans la deuxième partie, afin de mieux comprendre l’effet de l’hydrogène et de la dilution dans un moteur à combustion interne et leurs influences sur les propriétés fondamentales de la combustion, la vitesse de combustion laminaire, paramètre fondamentale, a été déterminée expérimentalement pour des mélanges isooctane ou méthane avec de l’air contenant différents pourcentages d’hydrogène et de dilution. Des corrélations ont pu ainsi être formulées permettant d’estimer la vitesse fondamentale de combustion laminaire pour ces mélanges. Dans la dernière partie, l’utilisation de deux diagnostics optiques (la chemiluminescence de la flamme et la tomographie par plan laser du front de flamme couplé à la mesure de vitesse par vélocimétrie par imagerie de particules) a permis de quantifier l’effet de l’hydrogène et de la dilution sur la propagation de flamme turbulente dans un moteur à allumage commandé muni d’accès optiques. Nous avons ainsi montré que le la vitesse de combustion laminaire a un effet prépondérant, comparé au nombre de Lewis, sur la vitesse de combustion turbulente dans un moteur à allumage commandé. / Optimization of the intake air-fuel mixture composition is one way to reduce pollutant emissions in Spark-Ignition (SI) engines. This can be achieved by operating with a diluted mixture, i.e by recirculating the exhaust. There are however limitations on the level of dilution that can ensure the smooth running of SI engines since diluting the air-fuel mixture induces an increase in combustion duration and in cyclic variations which impair engine performance. Adding an amount of hydrogen to the fuel can extend the dilution and the lean engine operability limits, which is beneficial in reducing both emission levels and fuel consumption. The objective of this study is to investigate the combined effects of hydrogen addition and nitrogen dilution in an SI engine fuelled with iso-octane or methane. In the first part of this study, we proved that high values of indicated engine efficiency and low values of pollutant emissions can be achieved by combining hydrogen addition and diluted air-fuel mixtures in the case of SI engines. In the second part, we provided experimental values of laminar burning velocity for diluted methane or iso-octane/hydrogen/air mixtures for a better understanding of the hydrogen and dilution effects on the fundamental properties of laminar combustion. New correlations to estimate laminar burning speeds of these mixtures were also presented. In the last part, the effects of hydrogen addition, with and without nitrogen dilution, on the turbulent flame propagation were investigated in an optical SI engine fuelled with iso-octane or methane. This study was done by using two different experimental techniques (direct flame radiation visualization and laser tomography images with Particle Image Velocimetry). The main conclusion is that the laminar burning velocity, rather than the Lewis number, has the dominant effect on the turbulent burning velocity in an SI engine.

Producer gas derived from biomass is one of the most environment friendly substitutes to the fossil fuels. Usage of producer gas for power generation has effect of zero net addition of CO2 in atmosphere. The engines working on producer gas have potential to decrease the dependence on conventional fuels for power generation. However, the combustion process is governed by complex interactions between chemistry and fluid dynamics, some of which are not completely understood. Improved knowledge of combustion is, therefore, of vital importance for both direct use in the design of engines, and for the evolution of reliable simulation tools for engine development. The present work is related to the turbulent combustion of producer gas in closed vessels and engine cylinders. The main objective of the work was multi-dimensional simulation of turbulent combustion in the bowl-in-piston engine operating on producer gas fuel and to observe the flame and flow field interaction. First, the combustion model was validated in constant volume combustion chamber with experimental results. Experimental turbulent combustion data of producer gas (composition matching with engine operating conditions) was presented. The required data of laminar burning velocity of producer gas was computed and used in the simulation of turbulent combustion in closed vessel. The effect of squish and reverse squish flow on flame propagation in the bowl-in-piston engine cylinder was described. Laminar burning velocity of unstretched flame was computed using flame code which was developed earlier in this laboratory. One dimensional computations of unstretched planar flame were made to calculate laminar burning velocity of the producer gas-air mixture at pressures (1-10 bar) and temperatures (300-600 K). A correlation of laminar burning velocity of producer gas as a function of pressure and temperature was fitted and compared with experiments. A fixed composition and equivalence ratio of producer gas-air mixture, typical of the engine operating conditions, was considered. The correlation was used in simulation of turbulent combustion in closed vessel. The turbulent combustion experiments with producer gas-air mixture were conducted in a closed vessel. The aim of experiments was to generate pressure-time data, in closed vessel during turbulent flame propagation, which was required to validate turbulent combustion models. Determination of (ST /SL) was made from pressure-time data which requires corresponding laminar combustion data with same initial conditions. For this purpose a set of laminar combustion experiments was conducted. Experimental setup consists of a constant volume combustion chamber of cubical shape and size 80 x 80 x 80 mm3 . The initial mixtures pressure and temperature were 1 bar and 300 K respectively. A fixed composition and equivalence ratio of producer gas-air mixture, typical of the engine operating conditions, was used. The composition of producer gas was H2 -19.61%, CO2 -19.68%, CH4 -2.52%, CO2 -12.55% and N2 -45.64% on volume basis. Fuel-air mixture was ignited with electric spark at the center of the cube. Initial turbulence in the chamber was created by moving a perforated plate with specified velocity. Perforated plate was placed in chamber so that the central hole in the plate passes over the spark electrodes as it sweeps across the chamber. Two geometrically similar plates with hole diameter of 5 and 10 mm were used. The new experimental setup constructed as a part of this work was first tested with one set of experiments each with methane and propane data of SL and ST /SL from the literature. Maximum turbulent intensity (u’) achieved was 1.092 ms−1 . The ratios of turbulent to laminar burning velocity (ST /SL) values were determined at six different turbulence intensity levels. Laminar combustion experiments were extended to elevated initial pressures 2-5 bar and temperature 300 K. The value of SL was calculated from the pressure-time history recorded during laminar stretching flame propagation inside closed vessel. These SL values were compared with computed SL,∞ after accounting for stretch. Turbulent combustion simulations were carried out to validate combustion models suitable for multi-dimensional CFD simulation of combustion in constant volume closed chamber. Two models proposed by Choi and Huh, based on Flame Surface Density (FSD) were tested with the present experimental results. User FORTRAN code for the source terms in transport equation of FSD was implemented in ANSYS-CFX 10.0 software. First model called CFM1, grossly under-predicted the rate of combustion. The second model called CFM2, predicted the results satisfactorily after replacing the arbitrary length scale with turbulent integral length scale (lt) having a limiting value near the wall. The modified CFM2 model was able to predict the propagation phase of the developed flame satisfactorily, though the duration for initial flame development was over-predicted by the model. CFD simulation of producer gas engine combustion process was carried out using ANSYSCFX software. Mesh deformation option was used to take care of moving boundaries such as piston and valve surfaces. The fluid domain expands during suction process and contracts during compression process. In order to avoid excessive distortion of the mesh elements, a series of meshes at different crank angle positions were generated and checked for their quality during mesh motion in the solver. For suction process simulation, unstructured meshes having 0.1 to 0.3 million cells were used. During the compression and combustion process simulations, structured meshes having 40,000 to 0.1 million cells were used. k-ε model was used for turbulence simulation. The suction, compression and combustion processes of an SI engine were simulated. Initial flame kernel was given by providing high flame surface density in a small volume comparable to the spark size at the time of ignition. The flame surface density model, CFM-2, was adapted with the modification of length scale tested against constant volume experiments. A suitable limiting value was used to avoid abnormal flame propagation near the wall. The limiting value of integral length scale (lt) near the wall was determined by linear extrapolation of the integral length scale in the domain to the wall. Engine p - θ curves of three different ignition timings 26°, 12° and 6°before top dead center (TDC) were simulated and compared with earlier experimental results. The effects of flow field on flame propagation have been observed. A comparison of the simulated and experimental p - θ diagram of the engine for all above cases gave mixed results. For the ignition timing at 26° before TDC case, predicted peak pressure value was 17% higher and at 3° earlier than those of the experimental peak. For the other two cases, the predicted peak pressure value was 28% lower and 5° later than those of the experimental peak. The reason for under-prediction of the pressure values could be due to the delay in development of initial flame kernel. Simulated pressure curves have offset about 3-4° compared to the experimental pressure curves. It was observed that in all predicted p - θ cases, there was a delay in the initial flame development. It is evident from the under-prediction of pressure values, especially in the initial flame kernel development phase and it also affects the p - θ curve at later stage. The delay was about 3-4° of crank angle rotation in various cases. The delay in predicting the initial flame development needs to be corrected in order to predict the combustion process properly. The proposed FSD model seems to have capability to predict p - θ values fairly in the propagation phase of developed flame. Reasonably good match was obtained by advancing the ignition timing in the computation by about 3-4° compared to the experimental setting. In the bowl-in-piston engine cylinders, the flow in the cylinder is characterised by squish and reverse squish when the piston is moving towards and away from the top dead center (TDC) respectively. The effect of squish and reverse squish flow on flame propagation has been assessed. For the more advanced ignition case, i.e., 26° before TDC, The flame propagation did not have favorable effect by the flow field. The direction of flame propagation was against the squish and reverse squish flow. This resulted in suppressed peak velocities in the cylinder compared the motoring process. Hence the burning rate was not augmented by the turbulence inside the cylinder. For the ignition 12° before TDC case, the flame propagation did have favorable effect by the flow field. During the reverse squish period, the flame had reached the bowl wall. At this stage, the flame was pushing the reactants out and this augments the reverse-squish flow, and hence the maximum reverse-squish velocity was increased to 2.03 times the peak reverse-squish velocity of motoring case. The reverse-squish flow was distorting the flame from spherical shape and the flame gets stretched. Flame surface enters the cylindrical region faster compared to the previous case. The stretched flame in the reverse-squish flow may be considered as reverse squish flame, as was proposed earlier by Sridhar G. The burn rate during the reverse squish period may be 2 to 2.5 times the normal burn rate. For the ignition 6° before TDC case, the flame was very small in size and it did not affect the flow in squish period. During the reverse squish period, the flame radius was moderate compared to the bowl radius. The flame was pushing the reactants out and it increased the maximum reverse-squish velocity to 1.3 times by the flame. In this case, the reverse-squish flow moderately affecting the flame shapes. The results of this study could give an idea of what ignition timing must be kept for favorable use of flow field inside the engine cylinder. Main contributions from the present work are: Multi-dimensional simulation of combustion process inside the engine cylinder operating on producer gas was carried out to examine flame/flow field interactions. Two models based on FSD were first tested against present experimental results in constant volume combustion chamber. In CFM2 model; a modification of replacing the arbitrary length scale by integral length scale with a limiting value near the wall was suggested to avoid prediction of abnormally large turbulent burning velocity near the wall. This combustion model has been implemented in ANSYS-CFX10. The required data of laminar and turbulent burning velocities of producer gas-air mixture has been determined by experiments and computations at varied initial pressures and turbulent intensities. Finally, the simulated engine pressure data has been compared with earlier experimental data of the engine operating on producer gas. The proposed FSD model has the capability to match well with the experimental results except for the initial flame kernel development phase. Even though this issue needs to be resolved, the work has brought out the important interaction between the flame propagation and flow field within the bowl-in-piston engine cylinder.

Face aux normes actuelles et futures de plus en plus draconiennes en termes d’émissions polluantes, les constructeurs automobiles cherchent en permanence à améliorer le rendement des moteurs à allumage commandé. L’une des voies efficaces et applicables à court terme pour réduire les émissions de dioxyde de carbone (CO2) consiste à réduire la cylindrée des moteurs tout en conservant leur performance grâce à la sur-alimentation : c’est l’approche de l’éco-suralimentation ou « downsizing ». L’une des particularités de ce mode de fonctionnement est le fort niveau de pression et de taux de dilution dans lequel se propage la flamme de prémélange. La simulation de la combustion turbulente de prémélange est devenue un outil incontournable pour la R&D. Toutefois, les hypothèses sur lesquelles reposent les modèles de combustion, tout particulièrement le modèle de flammelettes, peuvent être sujettes à discussion dans le cas d’un fonctionnement de type « downsizing ». Le but de ce travail de thèse est donc d’étudier expérimentalement les régimes de combustion de manière à valider ou non l’utilisation de ces modèles. Les grandeurs caractéristiques de la turbulence ont alors été caractérisées lors de la phase de compres-sion pour différentes pressions d’admission à l’aide de la vélocimétrie par imagerie de particules. La vitesse de combustion de laminaire a, quant à elle, été estimée à partir d’un mécanisme cinétique réduit. L’utilisation de la tomographie laser par diffusion de Mie avec et sans suivi temporel, nous a permis de caractériser la vitesse de combustion turbulente et la structure du front de flamme pour différentes pressions d’admission et différents taux de dilution. Lors de cette étude, nous avons ainsi pu mettre en évidence une cassure dans l’évolution de la PMI et de la vitesse de combustion turbulente à partir d’un taux de dilution de 25% : cette cassure a été reliée à la transition entre le régime de flammelette et le régime des flammes plissées épaissies. / Faced with the current and future more and more drastic standards for pollutant emissions, car manufacturers try to improve the efficiency of Spark Ignition engine. One effective and applicable ways to reduce the greenhouse emissions (CO2) in the short run is based on the reduction of the engine size while preserving their performance thank to turbocharging: eco-supercharging or « downsizing » approaches. One of the characteristics of this operating mode is the high level of the pressure and of the dilution rate of the medium in which the premixed flame propagates. The simulation of turbulent premixed flame is nowadays an indispensable tool for R&D. However, the assumptions on which the combustion models are based, particularly the flamelet model, can be prone to discussion in the « downsizing » conditions. The objective of this work is thus to study experimentally the combustion regimes in order to validate or not the use of these models. Turbulence parameters and flow fields were then characterized out during the compression stroke for several intake pressures by using Particle Imaging Velocimetry technique. The laminar burning velocity was estimated by using reduced chemical kinetic schemes. The Mie scattering laser tomography technique with and without temporal follow-up, enabled us to characterize the turbulent burning velocity and the flame front structure for different intake pressures and dilution rates. In this study, a break in the evolution of the IMEP and the turbulent burning velocity for a dilution rate of 25% has been obtained: this break was linked to the transition between the flamelet zone and the distributed reaction zones.

Depuis plusieurs années, les constructeurs automobiles suivent la voie du « downsizing » pour le développement des moteurs à allumage commandé. Ce procédé basé sur la réduction des cylindrées moteur combinée à la suralimentation a déjà fait ses preuves quant à son intérêt dans l’augmentation du rendement et la réduction des émissions polluantes des moteurs à essence. Les nouvelles conditions thermodynamiques, de turbulence et de dilution de ces moteurs engendrant de nouvelles possibilités de dilution dans les mélanges air/carburant, elles amènent également de nouvelles problématiques quant aux combustions anormales observées et l’apparition d’importantes variabilités cycliques. Ces travaux de thèse s’insèrent dans l’objectif de compréhension du comportement des flammes de prémélange d’isooctane/air en expansion dans des conditions représentatives d’un moteur « downsizé ». Leur étude a dans un premier temps été réalisée dans des conditions laminaires afin d’extraire les vitesses de flammes et longueurs de Markstein associées aux différents mélanges réactifs, et notamment sous forte dilution. Des corrélations ont alors été développées pour répondre aux besoins des modèles de simulation. Un nouveau dispositif de diagnostic optique a ensuite été employé pour améliorer la visualisation des flammes turbulentes en expansion. Une corrélation de coefficient correctif est ici développée pour remédier à la surestimation de vitesse engendrée par une visualisation Schlieren de ces flammes turbulentes. Une étude approfondie de l’influence des conditions thermodynamiques initiales, de la turbulence, ainsi que des caractéristiques diffusives du mélange air/carburant a par ailleurs été conduite afin d’isoler l’effet de chacun de ces paramètres sur le développement et la propagation de la flamme turbulente. Enfin l’effet d’une évolution simultanée des conditions thermodynamiques initiales similaire à celle d’une compression moteur a été étudié pour mieux appréhender les changements de comportement des flammes turbulentes dans des conditions plus représentatives du moteur à allumage commandé. / For several years, “downsizing” is used by car manufacturers to develop new spark ignition engines. This method based on the reduction of engine size combined with an increase of intake pressure (turbocharger) is well known to reduce pollutant emissions and increase efficiency. New thermodynamic, turbulent and dilution conditions could be used with these new engines but they can bring new issues like unusual combustion or cyclic variability. This thesis took place to improve the understanding of premixed expanding isooctane/air flames behavior under downsized engine-like conditions. As a first step, this work is conducted under laminar conditions to extract laminar burning velocities and Markstein lengths of the different mixtures, especially under high dilution. New correlations are then developed to answer the needs of numerical models. A new optical dispositive is then used to improve the visualization of turbulent expanding flames. A corrective coefficient correlation is proposed to avoid the overestimated values of turbulent burning speed generated by Schlieren visualization with such turbulent flames. A deep survey of starting conditions (temperature, pressure, turbulence, dissipative characteristics of air/fuel mixtures) influence is done to investigate the effect of each parameters on the development and the propagation of the turbulent flame. Finally, the effect of a coupled rise of initial temperature and pressure, similar to an engine compression, is studied to better understand the changes of flame behavior under more realistic spark-ignition engine conditions.

Spark ignited engines are still important for conventional as well as for hybrid power trains and are thus objective to optimization. Today a lot of functionalities arise from software solutions, which have to be calibrated. Modern engine technologies provide an extensive variability considering their valve train, fuel injection and load control. Thus, calibration efforts are really high and shall be reduced by introduction of virtual methods. In this work a physical 0D combustion model is set up, which can cope with a new generation of spark ignition engines. Therefore, at first cylinder thermodynamics are modeled and validated in the whole engine map with the help of a real-time capable approach. Afterwards an up to date turbulence model is introduced, which is based on a quasi-dimensional k-epsilon-approach and can cope with turbulence production from large scale shearing. A simplified model for ignition delay is implemented which emphasizes the transfer from laminar to turbulent flame propagation after ignition. The modeling is completed with the calculation of overall heat release rates in a 0D entrainment approach with the help of turbulent flame velocities. After validation of all sub-models, the 0D combustion prediction is used in combination with a 1D gas exchange analysis to virtually calibrate the modern engine torque structure and the ECU function for exhaust gas temperature with extensive simulations. / Moderne Ottomotoren spielen heute sowohl in konventionellen als auch hybriden Fahrzeugantrieben eine große Rolle. Aktuelle Konzepte sind hochvariabel bezüglich Ventilsteuerung, Kraftstoffeinspritzung und Laststeuerung und ihre Optimierungspotentiale erwachsen zumeist aus neuen Softwarefunktionen. Deren Applikation ist zeit- und kostenintensiv und soll durch virtuelle Methoden unterstützt werden. In der vorliegenden Arbeit wird ein physikalisches 0D Verbrennungsmodell für Ottomotoren aufgebaut und bis zur praktischen Anwendung geführt. Dafür wurde zuerst die Thermodynamik echtzeitfähig modelliert und im gesamten Motorenkennfeld abgeglichen. Der Aufbau eines neuen Turbulenzmodells auf Basis der quasidimensionalen k-epsilon-Gleichung ermöglicht anschließend, die veränderlichen Einflüsse globaler Ladungsbewegung auf die Turbulenz abzubilden. Für den Brennverzug wurde ein vereinfachtes Modell abgeleitet, welches den Übergang von laminarer zu turbulenter Flammenausbreitung nach der Zündung in den Vordergrund stellt. Der restliche Brennverlauf wird durch die physikalische Ermittlung der turbulenten Brenngeschwindigkeit in einem 0D Entrainment-Ansatz dargestellt. Nach Validierung aller Teilmodelle erfolgt die virtuelle Bedatung der Momentenstruktur und der Abgastemperaturfunktion für das Motorsteuergerät.