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Shock Tube Measurement of Ethylene Ignition Delay Time and Molecular Collision Theory Analysis
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作者 Xiao-he Xiong Yan-jun Ding +1 位作者 Shuo Shi Zhi-min Peng 《Chinese Journal of Chemical Physics》 SCIE CAS CSCD 2016年第6期761-766,I0002,共7页
In this study, 75% and 96% argon diluent conditions were selected to determine the ig- nition delay time of stoichiometric mixture of C2Ha/O2/Ar within a range of pressures (1.3-:3.0 arm) and temperatures (1092-17... In this study, 75% and 96% argon diluent conditions were selected to determine the ig- nition delay time of stoichiometric mixture of C2Ha/O2/Ar within a range of pressures (1.3-:3.0 arm) and temperatures (1092-1743 K). Results showed a logarithmic linear rela- tionship of the ignition delay time with the reciprocal of temperatures. Under both two diluent conditions, ignition delay time decreased with increased temperature. By multiple linear regression analysis, the ignition delay correlation was deduced. According to this correlation, the calculated ignition delay time in 96% diluent was found to be nearly five times that in 75% diluent. To explain this discrepancy, the hard-sphere collision theory was adopted, and the collision numbers of ethylene to oxygen were calculated. The total collision numbers of ethylene to oxygen were 5.99×10^30 s^-1cm^-3 in 75% diluent and 1.53×10^29 s^-1cm^-3 in 96% diluent (about 40 times that in 75% diluent). According to the discrepancy between ignition delay time and collision numbers, viz. 5 times corresponds to 40 times, the steric factor can 展开更多
关键词 shock tube ethylene ignition delay Molecule collision
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Shock tube study of kerosene ignition delay at high pressures 被引量:13
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作者 LIANG JinHu WANG Su +3 位作者 HU HongHao ZHANG ShengTao FAN BingCheng CUI JiPing 《Science China(Physics,Mechanics & Astronomy)》 SCIE EI CAS 2012年第6期947-954,共8页
Ignition delay times of China No.3 aviation kerosene were measured behind reflected shock waves using a heated high-pressure shock tube.Experimental conditions covered a wider temperature range of 820-1500 K,at pressu... Ignition delay times of China No.3 aviation kerosene were measured behind reflected shock waves using a heated high-pressure shock tube.Experimental conditions covered a wider temperature range of 820-1500 K,at pressures of 5.5,11 and 22 atm,equivalence ratios of 0.5,1.0 and 1.5,and oxygen concentration of 20%.Adsorption of kerosene on the shock tube wall was taken into account.Ignition delay times were determined from the onset of the excited radical OH emission in conjunction with the pressure profiles.The experimental results of ignition delay time were correlated with the equations:11 0.22 1.09 2 3.2 10 [Keros ene ] [O2] exp(69941 RT) and 7 0.88 0.23 4.72 10 P exp(62092 RT).The current measurements provide the ignition delay behavior of China No.3 aviation kerosene at high pressures and air-like O2 concentration. 展开更多
关键词 ignition delay time KEROSENE shock tube high pressure
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Shock tube study of n-decane ignition at low pressures 被引量:2
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作者 Xiao-Fei Nie Ping Li +3 位作者 Chang-Hua Zhang Wei Xie Cong-Shan Li Xiang-Yuan Li 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2012年第1期79-82,共4页
Ignition delay times for n-decane/O2/Ar mixtures were measured behind reflected shock waves using endwall pressure and CH* emission measurements in a heated shock tube. The initial postshock conditions cover pressure... Ignition delay times for n-decane/O2/Ar mixtures were measured behind reflected shock waves using endwall pressure and CH* emission measurements in a heated shock tube. The initial postshock conditions cover pressures of 0.09-0.26 MPa, temperatures of 1 227-1 536 K, and oxygen mole fractions of 3.9%-20.7% with an equivalence ratio of 1.0. The correlation formula of ignition delay dependence on pressure, temperature, and oxygen mole fraction was obtained. The current data are in good agreement with available low-pressure experimental data, and they are then compared with the prediction of a kinetic mechanism. The current measurements extend the kinetic modeling targets for the n-decane combustion at low pressures. 展开更多
关键词 ignition delay time n-Decane Heated shock tube
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Auto-ignition of biomass synthesis gas in shock tube at elevated temperature and pressure 被引量:2
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作者 Linqi Ouyang Hua Li +2 位作者 Shuzhou Sun Xiaole Wang Xingcai Lu 《Science Bulletin》 SCIE EI CAS CSCD 2015年第22期1935-1946,共12页
Ignition delay times of multi-component biomass synthesis gas (bio-syngas) diluted in argon were measured in a shock tube at elevated pressure (5, 10and 15 bar, 1 bar = 105 Pa), wide temperature ranges (1,100-1,7... Ignition delay times of multi-component biomass synthesis gas (bio-syngas) diluted in argon were measured in a shock tube at elevated pressure (5, 10and 15 bar, 1 bar = 105 Pa), wide temperature ranges (1,100-1,700 K) and various equivalence ratios (0.5, 1.0, 2.0). Additionally, the effects of the variations of main constituents (H2:CO = 0.125-8) on ignition delays were investigated. The experimental results indicated that the ignition delay decreases as the pressure increases above certain temperature (around 1,200 K) and vice versa. The ignition delays were also found to rise as CO concentration increases, which is in good agreement with the literature. In addition, the ignition delays of bio-syngas were found increasing as the equivalence ratio rises. This behavior was primarily discussed in present work. Experimental results were also compared with numerical predictions of multiple chemical kinetic mechanisms and Li's mechanism was found having the best accuracy. The logarithmic ignition delays were found nonlinearly decrease with the H2 concentration under various conditions, and the effects of temperature, equivalence ratio and H2 concentration on the ignition delays are all remarkable. However, the effect of pressure is rela- tively smaller under current conditions. Sensitivity analysis and reaction pathway analysis of methane showed that R1 (H +O2= O -9 OH) is the most sensitive reaction promot- ing ignition and R13 (H +O2 (+M) = HO2 (+M)), R53(CH3+H (+M)= CH4 (+M)), R54 (CH4+H= CH3 + H2) as well as R56 (CH4 + OH = CH3 + H2O) are key reactions prohibiting ignition under current experimental conditions. Among them, R53 (CH3 + H (+M) = CH4 (+M)), R54 (CH4 + H = CH3 + H2) have the largest posi- tive sensitivities and the high contribution rate in rich mixture. The rate of production (ROP) of OH of R1 showed that OH ROP of R1 decreases sharply as the mixture turns rich. Therefore, the ignition delays become longer as the equiva- lence ratio increases. 展开更多
关键词 shock tube Biomass synthesis gas ignition delay time Sensitivity analysis Reactionpathway analysis
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Effect of 2,5-dimethylfuran addition on ignition delay times of n-heptane at high temperatures 被引量:4
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作者 Zhenhua GAO Erjiang HU +2 位作者 Zhaohua XU Geyuan YIN Zuohua HUANG 《Frontiers in Energy》 SCIE CSCD 2019年第3期464-473,共10页
The shock tube autoignition of 2,5-dimethylfuran (DMF)/n-heptane blends (DMF)/n-100%, by mole fraction) with equivalence ratios of 0.5, 1.0, and 2.0 over the temperature range of 1200-1800 K and pressures of 2.0 atm a... The shock tube autoignition of 2,5-dimethylfuran (DMF)/n-heptane blends (DMF)/n-100%, by mole fraction) with equivalence ratios of 0.5, 1.0, and 2.0 over the temperature range of 1200-1800 K and pressures of 2.0 atm and 10.0 atm were investigated. A detailed blend chemical kinetic model resulting from the merging of validated kinetic models for the components of the fuel blends was developed. The experimental observations indicate that the ignition delay times nonlinearly increase with an increase in the DMF addition level. Chemical kinetic analysis including radical pool analysis and flux analysis were conducted to explain the DMF addition effects. The kinetic analysis shows that at lower DMF blending levels, the two fuels have negligible impacts on the consumption pathways of each other.As the DMF addition increases to relatively higher levels, the consumption path of n-heptane is significantly changed due to the competition of small radicals, which primarily leads to the nonlinear increase in the ignition delay times of DMF/n-heptane blends. 展开更多
关键词 ignition delay time shock tube KINETIC model 2 5-dimethylfuran (DMF) N-HEPTANE
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The vitiation effects of water vapor and carbon dioxide on the autoignition characteristics of kerosene
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作者 Jin-Hu Liang Su Wang +4 位作者 Sheng-Tao Zhang Lian-Jie Yue Bing-Cheng Fan Xin-Yu Zhang Ji-Ping Cui 《Acta Mechanica Sinica》 SCIE EI CAS CSCD 2014年第4期485-494,共10页
In ground tests of hypersonic scramjet, the highenthalpy airstream produced by burning hydrocarbon fuels often contains contaminants of water vapor and carbon dioxide. The contaminants may change the ignition characte... In ground tests of hypersonic scramjet, the highenthalpy airstream produced by burning hydrocarbon fuels often contains contaminants of water vapor and carbon dioxide. The contaminants may change the ignition characteristics of fuels between ground tests and real flights. In order to properly assess the influence of the contaminants on ignition characteristics of hydrocarbon fuels, the effect of water vapor and carbon dioxide on the ignition delay times of China RP-3 kerosene was studied behind reflected shock waves in a preheated shock tube. Experiments were conducted over a wider temperature range of 800-1 500 K, at a pressure of 0.3 MPa, equivalence ratios of 0.5 and 1, and oxygen concentration of 20%. Ignition delay times were determined from the onset of the excited radical OH emission together with the pressure profile. Ignition delay times were measured for four cases: (1) clean gas, (2) gas vitiated with 10% and 20% water vapor in mole, (3) gas vitiated with 10% carbon dioxide in mole, and (4) gas vitiated with 10% water vapor and 10% carbon dioxide, 20% water vapor and 10% carbon dioxide in mole. The results show that carbon dioxide produces an inhibiting effect at temperatures below 1 300 K when Ф = 0.5, whereas water vapor appears to accelerate the ignition process below a critical temperature of about 1 000 K when Ф = 0.5. When both water vapor and carbon dioxide exist together, a minor inhibiting effect is observed at Ф = 0.5, while no effect is found at Ф = 1.0. The results are also discussed preliminary by considering both the combustion reaction mechanism and the thermophysics properties of the fuel mixtures. The current measurements demonstrate vitiation effects of water vapor and carbon dioxide on the autoignition characteristics of China RP-3 kerosene at air-like O2 concentration. It is important to account for such effects when data are extrapolated from ground testing to real flight conditions. 展开更多
关键词 ignition delay · Vitiation effect · Kerosene wa-ter · Carbon dioxide · shock tube
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低稀释度条件下乙烯点火特性的激波管研究 被引量:2
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作者 梁金虎 胡弘浩 +3 位作者 王苏 张胜涛 范秉诚 崔季平 《力学学报》 EI CSCD 北大核心 2014年第1期155-159,共5页
在激波管中利用反射激波后高温环境加热燃料,以燃料点火过程中氢氧自由基特征发射光谱强度的急剧变化作为点火发生的标志,在温度范围800~1650K,压力0.2MPa,0.7MPa,1.2MPa,化学当量比为0.5,1,2,O2浓度为空气含量20%的条件下,进行了C2H4/... 在激波管中利用反射激波后高温环境加热燃料,以燃料点火过程中氢氧自由基特征发射光谱强度的急剧变化作为点火发生的标志,在温度范围800~1650K,压力0.2MPa,0.7MPa,1.2MPa,化学当量比为0.5,1,2,O2浓度为空气含量20%的条件下,进行了C2H4/O2/Ar混合气在低稀释度条件下点火特性的实验研究.获得了乙烯点火延时随温度、压力、化学当量比、燃料以及氧化剂浓度等参数变化的拟合关系式.对乙烯点火转爆轰现象进行了初步观察,考察了初始温度对乙烯点火特性以及点火转爆轰的影响. 展开更多
关键词 点火延时 乙烯 爆轰 激波管
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空气污染组分H_2O和CO_2对乙烯点火特性的影响 被引量:3
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作者 梁金虎 胡弘浩 +3 位作者 王苏 张胜涛 范秉诚 崔季平 《推进技术》 EI CAS CSCD 北大核心 2014年第2期220-226,共7页
超燃研究地面实验中通过燃烧加热方式获得的高焓气体中通常含有H2O和CO2等污染组分,污染组分可能造成地面实验与天空飞行中燃料的点火特性出现差异。为了正确评估这两种污染组分对碳氢燃料点火特性的影响,在预加热激波管上研究了H2O和CO... 超燃研究地面实验中通过燃烧加热方式获得的高焓气体中通常含有H2O和CO2等污染组分,污染组分可能造成地面实验与天空飞行中燃料的点火特性出现差异。为了正确评估这两种污染组分对碳氢燃料点火特性的影响,在预加热激波管上研究了H2O和CO2对乙烯点火特性的影响效应。以压力0.2MPa,化学当量比1和0.5乙烯在纯净气体中点火特性为基础,分别进行了单独加入7.5%,15%和25%的H2O,单独加入10%的CO2,以及同时加入25%H2O+10%CO2条件下,污染组分对乙烯点火特性影响的对比实验研究。结果表明:在贫油条件下(Φ=0.5),单独污染组分H2O和CO2对乙烯的点火基本没有影响;在化学当量比条件下(Φ=1)时,H2O和CO2分别对乙烯的点火具有一定的阻滞作用;当H2O和CO2同时存在时,污染组分在较大温度范围内表现出对乙烯点火的阻滞作用。从燃烧反应机理和热物理性质的角度对实验结果进行了初步分析。 展开更多
关键词 污染效应 点火延时 乙烯 激波管
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基于激波管装置的乙烯氧化实验研究与动力学机理分析 被引量:2
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作者 熊小鹤 丁艳军 +2 位作者 操晓波 彭志敏 李永华 《物理化学学报》 SCIE CAS CSCD 北大核心 2016年第6期1416-1423,共8页
在乙烯/氧气化学计量比为1,温度1092-1743 K,压力1.3-3.0 atm(1 atm=101325 Pa)范围内,利用激波管测量了在摩尔分数为96%和75%两种不同氩气稀释度工况下的乙烯/氧气/氩气反应体系的着火延迟时间。实验结果表明,乙烯着火延迟时间在低稀... 在乙烯/氧气化学计量比为1,温度1092-1743 K,压力1.3-3.0 atm(1 atm=101325 Pa)范围内,利用激波管测量了在摩尔分数为96%和75%两种不同氩气稀释度工况下的乙烯/氧气/氩气反应体系的着火延迟时间。实验结果表明,乙烯着火延迟时间在低稀释度下比高稀释度下短,着火延迟时间的对数与温度的倒数成良好线性关系,随着温度增加着火延迟时间缩短。此外,低稀释度下,能观察到爆轰(或者爆燃转爆轰)现象,而在高稀释度下,未发生爆轰现象。将四种不同机理模拟结果与实验结果比较,发现LLNL机理与实验结果吻合得较好。反应路径分析研究表明,稀释度对乙烯氧化反应路径无影响,而温度影响较大,温度增加,乙烯消耗路径由四条减少为三条,反应C_2H_4+H(+M)=C_2H_5(+M)由正向消耗乙烯变为逆向生成乙烯。 展开更多
关键词 激波管 乙烯 着火延迟 爆燃 爆轰 氧化
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强点火条件下RP-3航空煤油燃爆特性实验研究 被引量:2
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作者 毛浩清 黄炜超 +1 位作者 李斌 解立峰 《高压物理学报》 EI CAS CSCD 北大核心 2018年第2期148-155,共8页
为进一步探究影响RP-3航空煤油燃爆特性参数的因素,在内径为200mm、高度为5 400mm的立式激波管中,采用强点火方式,测定了其在不同浓度下的临界起爆能以及不同起爆能量、浓度当量比、喷雾压力下RP-3航空煤油的爆速和爆压。实验结果表明:... 为进一步探究影响RP-3航空煤油燃爆特性参数的因素,在内径为200mm、高度为5 400mm的立式激波管中,采用强点火方式,测定了其在不同浓度下的临界起爆能以及不同起爆能量、浓度当量比、喷雾压力下RP-3航空煤油的爆速和爆压。实验结果表明:航空煤油的临界起爆能随浓度当量比的增加先急剧降低,达到最小值后又缓慢上升,基本呈"L"形变化;在喷雾压力为0.20~0.60MPa、同一浓度条件下,RP-3航空煤油的爆速、爆压随喷雾压力的变化曲线呈倒"U"形;随着起爆能量升高,爆速、爆压均呈直线上升趋势,并且当起爆能量小于1.68MJ/m^2时,煤油未达到直接爆轰状态;燃料的爆速、爆压随浓度当量比的增加先上升后下降,其变化趋势也基本呈倒"U"形。 展开更多
关键词 RP-3航空煤油 立式激波管 强点火 临界起爆能 爆速 爆压
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点火准则和稀释气体对乙烯点火延时的影响
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作者 刘二伟 徐胜利 《爆炸与冲击》 EI CAS CSCD 北大核心 2020年第6期12-20,共9页
利用矩形截面激波管研究点火准则和稀释气体对乙烯点火延时的影响。采用压电传感器记录测点压力时间历程,采用光谱仪和光电倍增管记录自发光强时间历程,以压力、总自发光强与·OH和·CH自由基特定能级发射光强等信号判定是否发... 利用矩形截面激波管研究点火准则和稀释气体对乙烯点火延时的影响。采用压电传感器记录测点压力时间历程,采用光谱仪和光电倍增管记录自发光强时间历程,以压力、总自发光强与·OH和·CH自由基特定能级发射光强等信号判定是否发生自点火,给出自点火过程的时间起始点和终止点,得到了不同点火准则和稀释气体对应的乙烯/氧气/氮气和乙烯/氧气/氩气点火延时。结果表明:相同工况的乙烯点火延时测量数据相对误差约为15%,数据验证了本文实验和测量方法可靠性。针对当量比为1.0、压力为0.2 MPa,得到了温度范围为905~1 489 K,稀释气体的摩尔分数为75%氮气和75%氩气时的乙烯点火延时,给出点火延时和温度拟合的Arrhenius型表达式。不同点火准则会影响所测点火延时数据,但多次测量结果确定的点火延时和温度变化规律近似相同。不同稀释气体对激波管自点火流场的影响表现为和流场均匀性以及混合物比热相关。相同工况的乙烯/氧气/氮气点火延时大于乙烯/氧气/氩气点火延时。高温区和低温区的乙烯/氧气/氩气点火延时与温度的拟合关系不同,转折温度约为1 121 K。 展开更多
关键词 点火延时 激波管 点火准则 稀释气体 乙烯
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乙烯/空气在激波管中自点火流场显示研究
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作者 刘二伟 徐胜利 《实验流体力学》 EI CAS CSCD 北大核心 2019年第1期62-71,共10页
为认识不同压力(p5)和温度(T5)的乙烯/空气自点火和火焰传播特征,在矩形激波管中,采用火焰自发光信号触发高速ICCD相机拍摄了反射激波后流场,得到了不同工况下乙烯/空气自点火流场序列图像。结果表明:对p5=106kPa,当T5=1210K,点火首先... 为认识不同压力(p5)和温度(T5)的乙烯/空气自点火和火焰传播特征,在矩形激波管中,采用火焰自发光信号触发高速ICCD相机拍摄了反射激波后流场,得到了不同工况下乙烯/空气自点火流场序列图像。结果表明:对p5=106kPa,当T5=1210K,点火首先发生在激波管反射端面附近,向上游(右侧)传播并形成近似平面火焰。火焰面随时间推进趋于垂直激波管轴线,火焰在传播过程中厚度近似保持不变,且内部存在漩涡结构。当降低T5,自点火位置逐渐远离反射端面,初始火焰厚度增大且光强变弱,由单个平面火焰演变为多个离散的不规则火焰。当T5=1077K,初始火焰首先出现在观察窗右侧(远离反射端面)并向上下游传播。当增大p5,火焰光强增大且漩涡尺寸减小,不同p5对应的火焰产生和传播规律类似。当p5=265和419kPa,火焰内部产生局部爆炸现象,多个局部爆炸区在传播过程中不断融合,最终形成向上游传播的近似平面火焰。 展开更多
关键词 激波管 乙烯 自点火 流场成像 火焰
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扩散时间对乙烯-空气燃爆特性的影响 被引量:1
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作者 杨理 饶国宁 +2 位作者 解立峰 王永旭 彭金华 《高压物理学报》 CAS CSCD 北大核心 2015年第5期369-376,共8页
为探究在有限空间中,初始压力为0.25MPa、两处乙烯气体瞬时源在不同扩散时间下的燃爆特性,在内径200mm、高5 400mm的立式激波管中,采用上下进气方式,在强起爆条件下,测定5个不同扩散时间下3种浓度的乙烯-空气混合气体(C2H4-Air)的燃爆... 为探究在有限空间中,初始压力为0.25MPa、两处乙烯气体瞬时源在不同扩散时间下的燃爆特性,在内径200mm、高5 400mm的立式激波管中,采用上下进气方式,在强起爆条件下,测定5个不同扩散时间下3种浓度的乙烯-空气混合气体(C2H4-Air)的燃爆参数。实验结果表明,扩散时间大于1h后,3种浓度的C2H4-Air混合气体燃爆参数趋于一致。4.00%(体积分数)C2H4-Air在当前实验条件下未能达到爆轰。6.67%C2H4-Air在5个扩散时间均可达到爆轰,扩散时间为1h时的爆压、爆速分别为4.24 MPa、1 719m/s。8.89%C2H4-Air在0.08h扩散时间下只发生爆燃,扩散时间为0.5h及以上发生爆轰,扩散时间为1h时的爆压、爆速分别为4.31 MPa、1 813m/s。通过烟熏技术捕捉到6.67%、8.89%的C2H4-Air混合气体的爆轰波胞格,胞格宽度分别为8.22、14.15mm,长宽比分别为1.44、1.57。 展开更多
关键词 气相爆轰 扩散时间 爆轰参数 立式激波管 直接起爆 胞格
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