An improved system for measuring the ignition energy of liquid fuel was built to perform experiments on aviation kerosene (Jet A). Compared to a previously used system (Shepherd et al. 1998), the present vessel has a more uniform temperature which can be held constant for long periods of time. This ensures thermal equilibrium of the liquid fuel and the vapor inside the vessel. A capacitive spark discharge circuit was used to generate damped sparks and an arrangement of resistors and measurement probes recorded the voltage and current histories during the discharge. This permitted measurement of the energy dissipated in the spark, providing a more reliable, quantitative measure of the ignition spark strength. With this improved system, the ignition energy of Jet A was measured at temperatures from 35C to 50C pressures from 0.300 bar (ambient pressure at 30 kft) to 0.986 bar (ambient pressure near sea level), mass-volume ratios down to 3 kg/m^3, with sparks ranging from 10 mJ to 0.3 J. Special fuel blends with flash points (Tfp) from 29C to 73.5C were also tested. The statistical properties of the ignition threshold energy were investigated using techniques developed for high-explosive testing. ududIgnition energy measurements at 0.585 bar with high mass-volume ratios (also referred to as mass loadings) showed that the trend of the dependence of ignition energy on temperature was similar for tests using the stored capacitive energy and the measured spark energy. The ignition energy was generally lower with the measured spark energy than with the stored spark energy. The present ignition energy system was capable of clearly resolving the difference in ignition energy between low and high mass-volume ratios. The ignition energy vs. temperature curve for 3 kg/m^3 was shifted approximately 5C higher than the curve for high mass-volume ratios of 35 kg/m^3 or 200 kg/m^3. The ignition energy was subsequently found to depend primarily on the fuel-air mass ratio of the mixture, although systematic effects of the vapor composition are also evident. As expected, the ignition energy increased when the initial pressure was raised from 0.585 bar to 0.986 bar, and decreased when the pressure was decreased to 0.3 bar. Finally, tests on special fuels having flash points different from that of commercial Jet A showed that the minimum ignition temperature at a spark energy of about 0.3 J and a pressure of 0.986 bar depends linearly on the flash point of the fuel.
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机译:建立了一种用于测量液体燃料着火能量的改进系统,以对航空煤油(Jet A)进行实验。与以前使用的系统相比(Shepherd等,1998),本容器的温度更加均匀,可以长时间保持恒定。这确保了液体燃料和容器内部的蒸气的热平衡。电容式火花放电电路用于产生阻尼火花,电阻器和测量探头的布置记录了放电期间的电压和电流历史。这允许测量火花中消散的能量,从而提供更可靠,定量的点火火花强度测量。使用改进的系统,可以在35°C至50°C的温度,0.300 bar(30 kft的环境压力)至0.986 bar(海平面附近的环境压力)的压力下,测量体积比低至3 kg / m ^ 3,火花范围为10 mJ至0.3J。还测试了闪点(Tfp)为29C至73.5C的特殊燃料混合物。使用为高爆炸试验开发的技术研究了点火阈值能量的统计特性。 在高体积比(也称为质量负载)下,在0.585 bar的点火能量测量表明,对于使用存储的电容能量和测得的火花能量的测试,点火能量对温度的依赖性趋势相似。所测量的火花能量的点火能量通常低于所存储的火花能量的点火能量。本发明的点火能量系统能够清楚地解决低和高质量比之间点火能量的差异。 3kg / m ^ 3的点火能量对温度的曲线比35kg / m ^ 3或200kg / m ^ 3的高体积比的曲线高约5℃。随后发现点火能量主要取决于混合物的燃料-空气质量比,尽管蒸汽成分的系统效果也很明显。如预期的那样,当初始压力从0.585 bar升高至0.986 bar时,点火能量增加,而当压力降至0.3 bar时,点火能量降低。最后,对闪点与商用喷气式飞机A的闪点不同的特殊燃料进行的测试表明,在约0.3 J的火花能量和0.986 bar的压力下,最低点火温度与燃料的闪点线性相关。
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