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FLAME STRUCTURE AND BURNING SPEED OF JP-10 AIR MIXTURES

机译:JP-10空气混合物的火焰结构和燃烧速度

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The burning speed and flame structure of Jet Propellant (JP)-10 fuel-air mixtures have been studied using two similar constant volumes: a cylindrical vessel with end windows and a spherical chamber. Both vessels are equipped with a central ignition, pressure transducer for measuring pressure rise during combustion process and ioniza-tion probes for monitoring flame arrival time. Both spherical and cylindrical chambers can be heated up to 500 K. The spherical vessel can withstand 425 atm pressures while the maximum allowable pressure for cylindrical chamber is 50 atm due to the two windows at end caps. A thermodynamic model has been developed to calculate burning speed using dynamic pressure rise in the spherical vessel. The model considers a central burned gas core of variable temperature surrounded by a preheat zone, an unburned gas shell with uniform temperature and a thermal boundary layer at the wall. The model also includes losses associated with thermal radiation from burned gas to the wall and heat losses to the electrodes and the wall. Measurements in the spherical chamber start when the flame radius is almost half of the chamber radius (about 3.8 cm), where ratio of flame radius to flame thickness is larger than 25, hence curvature and flame thickness effects can be neglected. Shadowgraph photographic observations were made through the end windows in the cylindrical chamber using a high-speed Charged Coupled Device (CCD) camera with variable speed of up to 8000 frames/second. Burning speeds of JP-10 air mixtures have been measured in a pressure range of 1-55 atm, temperature range of 450-700 K and equivalence ratios of 0.7-1. A correlation for burning speed as a function of temperature, pressure and equivalence ratio has been developed.
机译:已经使用两个相似的恒定体积研究了喷气推进剂(JP)-10燃料-空气混合物的燃烧速度和火焰结构:带端窗的圆柱形容器和球形腔。这两个容器都配备了中央点火,压力传感器,用于测量燃烧过程中的压力升高,以及电离探针,用于监控火焰的到达时间。球形腔室和圆柱形腔室都可以加热到500K。球形容器可以承受425 atm的压力,而圆柱形腔室的最大允许压力为50 atm,这是因为端盖上有两个窗口。已经开发出一种热力学模型来利用球形容器中的动态压力上升来计算燃烧速度。该模型考虑了一个中央温度可变的可燃气体核心,周围有一个预热区,一个温度均匀的未燃气体壳以及壁上的热边界层。该模型还包括与从燃烧气体到壁的热辐射以及到电极和壁的热损失相关的损失。当火焰半径几乎是腔室半径的一半(约3.8厘米)时,开始进行球形腔室的测量,此时,火焰半径与火焰厚度的比率大于25,因此可以忽略曲率和火焰厚度的影响。使用高速充电耦合设备(CCD)相机,以高达8000帧/秒的可变速度,通过圆筒形腔室中的端窗进行阴影照片摄影观察。 JP-10空气混合物的燃烧速度已在1-55 atm的压力范围,450-700 K的温度范围和0.7-1的当量比下进行了测量。已经开发出燃烧速度与温度,压力和当量比的关系。

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