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Diesel Engine has been the most powerful and relevant source of power in the automobile industryfor decades due to their excellent performance, efficiency and power. On the contrary, there arenumerous environmental issues of the diesel engines hampering the environment. It has been agreat challenge for the researchers and scientists to minimize these issues. In the recent years, severalstrategies have been introduced to eradicate the emissions of the diesel engines. Among them,Partially Premixed Combustion (PPC) is one of the most emerging and reliable strategies. PPC is acompression ignited combustion process in which ignition delay is controlled. PPC is intended toendow with better combustion with low soot and NOx emission.The engine used in the present study is a single-cylinder research engine, installed in Aalto UniversityInternal Combustion Engine Laboratory with the bore diameter of 200 mm. The thesis presentsthe validation of the measurement data with the simulated cases followed by the study of the sprayimpingement and fuel vapor mixing in PPC mode for different injection timing. A detailed study ofthe correlation of early injection with the fuel vapor distribution and wall impingement has beenmade.The simulations are carried out with the commercial CFD software STAR CD. Different injectionparameters have been considered and taken into an account to lower the wall impingement and toproduce better air-fuel mixing with the purpose of good combustion and reduction of the emissions.The result of the penetration length of the spray and the fuel vapor distribution for different earlyinjection cases have been illustrated in the study. Comparisons of different thermodynamic propertiesand spray analysis for different injection timing have been very clearly illustrated to get insightof effect of early injection. The parameters like injection timing, injection period, injection pressure,inclusion angle of the spray have an influence the combustion process in PPC mode. Extensivestudy has been made for each of these parameters to better understand their effects in the combustionprocess. Different split injection profiles have been implemented for the study of better fuelvapor distribution in the combustion chamber.The final part of the thesis includes the study of the combustion and implementation of EGR tocontrol the temperature so as to get more prolonged ignition delay to accompany the PPC strategyfor standard piston top and deep bowl piston top. With the injection optimization and implementationof EGR, NOx has been reduced by around 44%, CO by 60% and Soot by 66% in the standardpiston top. The piston optimization resulted in more promising result with 58% reduction in NOx,55% reduction in CO and 67% reduction in Soot. In both cases the percentage of fuel burnt wasincreased by around 8%.

Nos últimos anos o principal desafio da humanidade foi a substituição total ou parcial dos combustíveis fósseis que são responsáveis pelas mudanças climáticas e contribuem para a formação dos gases do efeito estufa. Como alternativa, os combustíveis renováveis - denominados biocombustíveis - têm se tornado uma alternativa viável. Este trabalho investigou o comportamento térmico e a energia de ativação de dois biocombustíveis (farnesano e biodiesel de soja) e suas misturas com diesel fóssil. Além disso, foram feitos estudos comparativos de comportamento térmico e energia de ativação entre todos os combustíveis. Os estudos foram feitos empregando-se análise termogravimétrica (TGA) sob atmosfera de ar sintético. As condições experimentais para os testes termogravimétricos foram: massa das amostras de 4,0 ± 0,5 mg, razões de aquecimento de 5, 10, 15, 20 e 25ºC min-1 e faixa de temperatura entre 30ºC e 400ºC. Outras técnicas, tais como calorimetria, Calorimetria Exploratória Diferencial (DSC - \"Differential Scanning Calorimetry\") e testes em motor diesel OM 926 LA CONAMA P7/EURO 5 também foram aplicadas para se avaliar o comportamento térmico destes combustíveis. Os valores de poder calorífico superior (PCS) para o farnesano, diesel fóssil e biodiesel são 46,9 MJ/kg, 45,3 MJ/kg e 39,7 MJ/kg, respectivamente. Os experimentos no motor diesel mostraram uma economia de 3% para o farnesano e um consumo de 14,25 % para o biodiesel em relação ao diesel fóssil. Em média, os valores de energia de ativação para os combustíveis puros encontrados neste estudo foram de 82,20 ± 3,38 kJ mol-1, 86,61 ± 8,48 kJ mol-1 e 96,61 ± 3,74 kJ mol-1 para farnesano, diesel fóssil e biodiesel de soja, respectivamente. Como a energia de ativação está diretamente relacionada com o atraso de ignição e, consequentemente, ao processo de combustão, o farnesano apresentou uma melhor qualidade de combustão em relação ao biodiesel de soja. Por meio das emissões obtidas nos testes European Stationary Cycle test (ESC) com a utilização do motor diesel foi possível obter correlações lineares entre energia de ativação e as emissões de óxidos de nitrogênio (NOx) e hidrocarbonetos (HC) e correlações polinomiais entre energia de ativação e as emissões de monóxido de carbono (CO), dióxido de carbono (CO2) e material particulado (MP). A adição de biodiesel de soja ao diesel provocou um aumento das emissões tanto para o NOx quanto para o HC em até 21,29% e 19,31%, respectivamente, e queda nas emissões de CO, CO2 e MP em até 33,44%, 2,44% e 47,37%, respectivamente. Por outro lado, a adição de farnesano ao diesel proporcionou uma diminuição de todas as emissões, ou seja, 11,22 %, 15,67%, 15,09%, 4,66% e 6,14% para NOx, HC, CO, CO2 e MP, respectivamente. A partir dos resultados obtidos neste estudo é possível entender o comportamento dos combustíveis durante suas respectivas queimas tendo como base as suas energias de ativação. / In recent years, the main challenge of the humanity was the total or partial replacement of fossil fuels, which are responsible for both the climate changes and the production of greenhouse gases. As an alternative, renewable fuels - named biofuels - have become viable. This study investigated the thermal behavior and the activation energy of two biofuels (farnesane and soybean biodiesel) and their mixture with fossil fuel. In addition, the thermal behavior of the biofuels and their mixtures with fossil fuel were compared with pure fossil diesel. Experiments were performed applying thermogravimetric analysis (TGA) under synthetic air atmosphere and other conditions such as, sample mass of 4,0 ± 0,5 mg, heating ratios of 5, 10, 15, 20 and 25 °C min-1 and temperature range between 30ºC and 400°C. In addition, calorimetry, differential scanning calorimetry (DSC) and experiments in a diesel engine OM 926 LA CONAMA P7 / EURO 5 were applied. Calorific value (CV) of the farnesane, biodiesel and fossil diesel are 46.9 MJ kg-1, 45.3 MJ kg-1 and 39.7 MJ kg-1, respectively. Experiments in the engine showed a fuel saving of 3% for farnesane and an increase consumption of 14.24 % for biodiesel, compared to fossil diesel. On average, the values of activation energy for pure fuels determined in this study were 82.20 ± 3.38 kJ mol-1, 86.61 ± 8.48 kJ mol-1 and 96.61 ± 3.74 kJ mol-1 for farnesane, fossil diesel and soybean biodiesel, respectively. As the activation energy is directly related to the ignition delay and hence the combustion process, it was observed that farnesane presented a better quality of combustion in comparison to the biodiesel. By means of the emissions obtained by the European Stationary Cycle test (ESC) in the diesel engine, it was possible to observe linear correlations between activation energy for both nitrogen oxide (NOx) and hydrocarbon (HC) emissions, and polynomial correlations between activation energy and carbon monoxide (CO), carbon dioxide (CO2) and particulate matter (PM) emissions. The addition of soybean biodiesel to the diesel promoted an increase of both NOx and HC emissions in 1.29% and 19.31%, respectively and a decrease of 33.44%, 2.44% and 47.37% for CO, CO2 and PM emissions, respectively. On the other hand, the addition of farnesane to the fossil diesel, a reduction in all emissions were observed, i.e, 11.22%, 16.67%, 15.09%, 4.66%, 6.14%. of NOx, HC, CO, CO2 and PM, respectively. From the results obtained in this study, it is possible to understand the behavior and the emissions of the fuels produced during their burning based on their activation energies.

In current afterburners combustion is stabilized by the high temperature, recirculating region behind bluff body flame holders, such as V-gutters. Blocking the high speed flow with bluff bodies causes a significant pressure drop, and heating the flame holder by the hot combustion product causes a thermal signature, which is a critical problem in a military jet. To reduce these problems, ignition methods using a high frequency (HF) spark discharge, or a radical jet generator (RJG) were developed. The HF discharge ignited and stabilized a flame successfully in a premixed methane-air flow. The electrical power consumption was very small compared to the combustion heat release, as long as the operating velocity was relatively low. However, a theoretical study showed that the ratio of the electrical power consumption to the heat generation by the stabilized flame increases rapidly with increasing flow velocity. For flame stabilization in a high velocity flow, the developed RJG showed much better performance than direct exposure to a plasma. The present study investigated the characteristics of a radical jet produced in a RJG and injected into a main combustor. The limits of flame stabilization by this jet was measured experimentally, and compared to those of bluff body flame holders. The flame holding performance of the radical jet was also experimentally compared to that of a thermal jet. The effect of radicals on flame stabilization was examined using CHEMKIN, and the limit of flame stabilization by the radical jet was estimated for a simple flow configuration using an approximate solution. The results suggest that the reduction of local spontaneous ignition delay time by active species in the radical jet and the longer length of a typical radical jet compared to the dimension of the recirculation zone behind a bluff body increases the maximum velocity at which a flame can be stabilized.

Applications of natural gases that contain high levels of hydrogen have become a primary interest in the gas turbine market. For reheat gas turbines, understanding of the ignition delay times of high-hydrogen natural gases is important for two reasons. First, if the ignition delay time is too short, autoignition can occur in the mixer before the primary combustor. Second, the flame in the secondary burner is stabilized by the ignition delay time of the fuel. While the ignition delay times of hydrogen and of the individual hydrocarbons in natural gases can be considered well known, there have been few previous experimental studies into the effects of different levels of hydrogen on the ignition delay times of natural gases at gas turbine conditions. In order to examine the effects of hydrogen content at gas turbine conditions, shock-tube experiments were performed on nine combinations of an L9 matrix. The L9 matrix was developed by varying four factors: natural gas higher-order hydrocarbon content of 0, 18.75, or 37.5%; hydrogen content of the total fuel mixture of 30, 60, or 80%; equivalence ratios of 0.3, 0.5, or 1; and pressures of 1, 10, or 30 atm. Temperatures ranged from 1092 K to 1722 K, and all mixtures were diluted in 90% Ar. Correlations for each combination were developed from the ignition delay times and, using these correlations, a factor sensitivity analysis was performed. It was found that hydrogen played the most significant role in ignition delay time. Pressure was almost as important as hydrogen content, especially as temperature increased. Equivalence ratio was slightly more important than hydrocarbon content of the natural gas, but both were less important than pressure or hydrogen content. Further analysis was performed using ignition delay time calculations for the full matrix of combinations (27 combinations for each natural gas) using a detailed chemical kinetics mechanism. Using these calculations, separate L9 matrices were developed for each natural gas. Correlations from the full matrix and the L9 matrix for each natural gas were found to be almost identical in each case, verifying that a thoughtfully prepared L9 matrix can indeed capture the major effects of an extended matrix.

Nos últimos anos o principal desafio da humanidade foi a substituição total ou parcial dos combustíveis fósseis que são responsáveis pelas mudanças climáticas e contribuem para a formação dos gases do efeito estufa. Como alternativa, os combustíveis renováveis - denominados biocombustíveis - têm se tornado uma alternativa viável. Este trabalho investigou o comportamento térmico e a energia de ativação de dois biocombustíveis (farnesano e biodiesel de soja) e suas misturas com diesel fóssil. Além disso, foram feitos estudos comparativos de comportamento térmico e energia de ativação entre todos os combustíveis. Os estudos foram feitos empregando-se análise termogravimétrica (TGA) sob atmosfera de ar sintético. As condições experimentais para os testes termogravimétricos foram: massa das amostras de 4,0 ± 0,5 mg, razões de aquecimento de 5, 10, 15, 20 e 25ºC min-1 e faixa de temperatura entre 30ºC e 400ºC. Outras técnicas, tais como calorimetria, Calorimetria Exploratória Diferencial (DSC - \"Differential Scanning Calorimetry\") e testes em motor diesel OM 926 LA CONAMA P7/EURO 5 também foram aplicadas para se avaliar o comportamento térmico destes combustíveis. Os valores de poder calorífico superior (PCS) para o farnesano, diesel fóssil e biodiesel são 46,9 MJ/kg, 45,3 MJ/kg e 39,7 MJ/kg, respectivamente. Os experimentos no motor diesel mostraram uma economia de 3% para o farnesano e um consumo de 14,25 % para o biodiesel em relação ao diesel fóssil. Em média, os valores de energia de ativação para os combustíveis puros encontrados neste estudo foram de 82,20 ± 3,38 kJ mol-1, 86,61 ± 8,48 kJ mol-1 e 96,61 ± 3,74 kJ mol-1 para farnesano, diesel fóssil e biodiesel de soja, respectivamente. Como a energia de ativação está diretamente relacionada com o atraso de ignição e, consequentemente, ao processo de combustão, o farnesano apresentou uma melhor qualidade de combustão em relação ao biodiesel de soja. Por meio das emissões obtidas nos testes European Stationary Cycle test (ESC) com a utilização do motor diesel foi possível obter correlações lineares entre energia de ativação e as emissões de óxidos de nitrogênio (NOx) e hidrocarbonetos (HC) e correlações polinomiais entre energia de ativação e as emissões de monóxido de carbono (CO), dióxido de carbono (CO2) e material particulado (MP). A adição de biodiesel de soja ao diesel provocou um aumento das emissões tanto para o NOx quanto para o HC em até 21,29% e 19,31%, respectivamente, e queda nas emissões de CO, CO2 e MP em até 33,44%, 2,44% e 47,37%, respectivamente. Por outro lado, a adição de farnesano ao diesel proporcionou uma diminuição de todas as emissões, ou seja, 11,22 %, 15,67%, 15,09%, 4,66% e 6,14% para NOx, HC, CO, CO2 e MP, respectivamente. A partir dos resultados obtidos neste estudo é possível entender o comportamento dos combustíveis durante suas respectivas queimas tendo como base as suas energias de ativação. / In recent years, the main challenge of the humanity was the total or partial replacement of fossil fuels, which are responsible for both the climate changes and the production of greenhouse gases. As an alternative, renewable fuels - named biofuels - have become viable. This study investigated the thermal behavior and the activation energy of two biofuels (farnesane and soybean biodiesel) and their mixture with fossil fuel. In addition, the thermal behavior of the biofuels and their mixtures with fossil fuel were compared with pure fossil diesel. Experiments were performed applying thermogravimetric analysis (TGA) under synthetic air atmosphere and other conditions such as, sample mass of 4,0 ± 0,5 mg, heating ratios of 5, 10, 15, 20 and 25 °C min-1 and temperature range between 30ºC and 400°C. In addition, calorimetry, differential scanning calorimetry (DSC) and experiments in a diesel engine OM 926 LA CONAMA P7 / EURO 5 were applied. Calorific value (CV) of the farnesane, biodiesel and fossil diesel are 46.9 MJ kg-1, 45.3 MJ kg-1 and 39.7 MJ kg-1, respectively. Experiments in the engine showed a fuel saving of 3% for farnesane and an increase consumption of 14.24 % for biodiesel, compared to fossil diesel. On average, the values of activation energy for pure fuels determined in this study were 82.20 ± 3.38 kJ mol-1, 86.61 ± 8.48 kJ mol-1 and 96.61 ± 3.74 kJ mol-1 for farnesane, fossil diesel and soybean biodiesel, respectively. As the activation energy is directly related to the ignition delay and hence the combustion process, it was observed that farnesane presented a better quality of combustion in comparison to the biodiesel. By means of the emissions obtained by the European Stationary Cycle test (ESC) in the diesel engine, it was possible to observe linear correlations between activation energy for both nitrogen oxide (NOx) and hydrocarbon (HC) emissions, and polynomial correlations between activation energy and carbon monoxide (CO), carbon dioxide (CO2) and particulate matter (PM) emissions. The addition of soybean biodiesel to the diesel promoted an increase of both NOx and HC emissions in 1.29% and 19.31%, respectively and a decrease of 33.44%, 2.44% and 47.37% for CO, CO2 and PM emissions, respectively. On the other hand, the addition of farnesane to the fossil diesel, a reduction in all emissions were observed, i.e, 11.22%, 16.67%, 15.09%, 4.66%, 6.14%. of NOx, HC, CO, CO2 and PM, respectively. From the results obtained in this study, it is possible to understand the behavior and the emissions of the fuels produced during their burning based on their activation energies.

Submitted by Edineia Teixeira (edineia.teixeira@unioeste.br) on 2018-09-21T18:57:27Z No. of bitstreams: 2 Paulo_Paiva_2018.pdf: 1808822 bytes, checksum: b60c2ed8673a5040b72da406c4cb66fd (MD5) license_rdf: 0 bytes, checksum: d41d8cd98f00b204e9800998ecf8427e (MD5) / Made available in DSpace on 2018-09-21T18:57:27Z (GMT). No. of bitstreams: 2 Paulo_Paiva_2018.pdf: 1808822 bytes, checksum: b60c2ed8673a5040b72da406c4cb66fd (MD5) license_rdf: 0 bytes, checksum: d41d8cd98f00b204e9800998ecf8427e (MD5) Previous issue date: 2018-03-16 / Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - CAPES / The tractor is the most used agricultural machine in the wide range of operations existing in the rural properties; being a source of mechanical energy for the operations, in which it is made available through the motor, this machine converts thermal energy into mechanics. In this context, the objective of this research was to evaluate the performance of the engine of an agricultural tractor using pure A-S500 diesel, binary (diesel-biodiesel) and ternary (diesel-biodiesel-ethanol) blends. In the case of a mechanical diesel fuel cycle engine, the injection time, known as the injection point, was also modified by changing it by 2 ° (P2), 4 ° (P4) and -2 ° (P-2), before and after the reference point of 0 ° (P0) (original of the motor), so that this moment is advanced and delayed in relation to the original. To evaluate the mechanical performance of the tractor, the data collected in this research were based on the use of a Foucault chain dynamometer coupled to the power take-off, in which the proposed diesel-biodiesel proportions were: B0, B8, B15 and B20, in (E0) and tests using the 1% (E1) ratio of this same substance. The dynamometric tests were performed with four replicates. As reference for the test and the analyzes was applied the condition B0P0E0, with 0.14% more B0P2E0 presented the best value for maximum power, B0E0P0 and B0E1P0 had the best torque values, in specific consumption B15E0P2 had a reduction of 17, 0%, already in consumption hour P-2 had better results being 10.1% of reduction. P-2 was the point of injection with better indexes of IE, RT and RR. / O trator é a máquina agrícola mais utilizada na grande gama de operações existentes nas propriedades rurais; sendo uma fonte de energia mecânica para as operações, na qual é disponibilizada por meio do motor, esta máquina converte energia térmica em mecânica. Neste contexto, esta pesquisa teve como objetivo avaliar o desempenho do motor de um trator agrícola, utilizando como combustíveis: o diesel puro A-S500, misturas binárias (diesel-biodiesel) e ternárias (diesel-biodiesel-etanol). E se tratando de um motor ciclo diesel de alimentação de combustível mecânica, o momento de injeção, conhecido como ponto de injeção também foi modificado, alterando-o em uma ordem de 2°(P2), 4°(P4) e -2°(P-2), antes e após ao ponto de referência de 0°(P0) (original do motor), sendo assim este momento adiantado e atrasado em relação ao original. Para avaliar o desempenho mecânico do trator, os dados coletados nesta pesquisa foram embasados na utilização de um dinamômetro de correntes de Foucault acoplado à tomada de potência, em que as proporções binarias diesel–biodiesel propostas foram: B0, B8, B15 e B20, nas quais ocorreram ensaios sem utilização de etanol (E0) e ensaios utilizando a proporção de 1%(E1) desta mesma substância. Os ensaios dinamométricos ocorreram com quarto repetições. Como referencial para o ensaio e as análises foi aplicado a condição B0P0E0, com 0,14% a mais B0P2E0 apresentou o melhor valor para potência máxima, B0E0P0 e B0E1P0 tiveram os melhores valores de torque, em consumo especifico B15E0P2 teve uma redução de 17,0%, já em consumo horário P-2 teve melhores resultados sendo 10,1% de redução.P-2 foi o ponto de injeçao com melhores índices de IE, RT e RR.

Indiana University-Purdue University Indianapolis (IUPUI) / Investigations of a constant-volume combustor ignited by a penetrating transient jet (a puff) of hot reactive gas have been conducted in order to provide vital data for designing wave rotor combustors. In a wave rotor combustor, a cylindrical drum with an array of channels arranged around the axis spins at a high rpm to generate high-temperature and high-pressure product gas. The hot-gas jet ignition method has been employed to initiate combustion in the channels. This study aims at experimentally investigating the ignition delay time of a premixed combustible mixture in a rectangular, constant-volume chamber, representing one channel of the wave rotor drum. The ignition process may be influenced by the multiple factors: the equivalence ratio, temperature, and the composition of the fuel mixture, the temperature and composition of the jet gas, and the peak mass flow rate of the jet (which depends on diaphragm rupture pressure). In this study, the main mixture is at room temperature. The jet composition and temperature are determined by its source in a pre-chamber with a hydrogen-methane mixture with an equivalent ratio of 1.1, and a fuel mixture ratio of 50:50 (CH4:H2 by volume). The rupture pressure of a diaphragm in the pre-chamber, which is related to the mass flow rate and temperature of the hot jet, can be controlled by varying the number of indentations in the diaphragm. The main chamber composition is varied, with the use of four equivalence ratios (1.0, 0.8, 0.6, and 0.4) and two fuel mixture ratios (50:50, and 30:70 of CH4:H2 by volume). The sudden start of the jet upon rupture of the diaphragm causes a shock wave that precedes the jet and travels along the channel and back after reflection. The shock strength has an important role in fast ignition since the pressure and the temperature are increased after the shock. The reflected shock pressure was examined in order to check the variation of the shock strength. However, it is revealed that the shock strength becomes attenuated compared with the theoretical pressure of the reflected shock. The gap between theoretical and measured pressures increases with the increase of the Mach number of the initial shock. Ignition delay times are obtained using pressure records from two dynamic pressure transducers installed on the main chamber, as well as high-speed videography using flame incandescence and Schileren imaging. The ignition delay time is defined in this research as the time interval from the diaphragm rupture moment to the ignition moment of the air/fuel mixture in the main chamber. Previous researchers used the averaged ignition delay time because the diaphragm rupture moment is elusive considering the structure of the chamber. In this research, the diaphragm rupture moment is estimated based on the initial shock speed and the longitudinal length of the main chamber, and validated with the high-speed video images such that the error between the estimation time and the measured time is within 0.5%. Ignition delay times decrease with an increase in the amount of hydrogen in the fuel mixture, the amount of mass of the hot-jet gases from the pre-chamber, and with a decrease in the equivalence ratio. A Schlieren system has been established to visualize the characteristics of the shock wave, and the flame front. Schlieren photography shows the density gradient of a subject with sharp contrast, including steep density gradients, such as the flame edge and the shock wave. The flame propagation, gas oscillation, and the shock wave speed are measured using the Schlieren system. An image processing code using MATLAB has been developed for measuring the flame front movement from Schlieren images. The trend of the maximum pressure in the main chamber with respect to the equivalence ratio and the fuel mixture ratio describes that the equivalence ratio 0.8 shows the highest maximum pressure, and the fuel ratio 50:50 condition reveals lower maximum pressure in the main chamber than the 30:70 condition. After the combustion occurs, the frequency of the pressure oscillation by the traversing pressure wave increases compared to the frequency before ignition, showing a similar trend with the maximum pressure in the chamber. The frequency is the fastest at the equivalence ratio of 0.8, and the slowest at a ratio of 0.4. The fuel ratio 30:70 cases show slightly faster frequencies than 50:50 cases. Two different combustion behaviors, fast and slow combustion, are observed, and respective characteristics are discussed. The frequency of the flame front oscillation well matches with that of the pressure oscillation, and it seems that the pressure waves drive the flame fronts considering the pressure oscillation frequency is somewhat faster. Lastly, a feedback mechanism between the shock and the flame is suggested to explain the fast combustion in a constant volume chamber with the shock-flame interactions.

A pulsed Nd:YAG laser is used to study laser spark ignition of methane counter-flow diffusion flames with the use of helium and argon as diluents to achieve a wide range of variations in transport properties. The global strain rate and Damkohler number on successful ignition were investigated for the effects of Lewis number and transport properties, which are dependent on the diluent type and dilution level. A high-speed camera is used to record the ignition events and a software is used for pre-ignition flow field and mixing calculations. It is found that the role of effective Lewis number on the critical global strain rate, beyond which ignition is not possible, is qualitatively similar that on the extinction strain rate. With the same level of dilution, the inert diluent with smaller Lewis number yields larger critical global strain rate. The critical Damkohler number below which no ignition is possible is found to be within approximately 20% for all the fuel-inert gas mixtures studied. When successful ignition takes place, the ignition time increases as the level of dilution of argon is increased. The ignition time decreases with increasing level of helium dilution due to decreases in thermal diffusion time, which causes rapid cooling of the flammable layer during the ignition process. However, the critical strain for ignition with helium dilution rapidly decreases as the dilution level is increased. The experimental results show that with the increase of strain rate the time to steady flame decreases, and that with the increase of dilution level time for the flame to become steady increases. For the same level of dilution, the time for steady flame is observed to be longer for He-diluted flames than for Ar-diluted flames due to its thermal diffusivity being larger than that of Ar.