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液氧相变膨胀气体的传播规律及压力分布特性

Propagation law and pressure distribution characteristics of liquid oxygen phase change expansion gas

  • 摘要: 针对不同液氧量对液氧瞬态相变膨胀效果的影响问题,通过高速纹影系统和超压检测系统对液氧相变膨胀产生的气体前沿与混合气体在自由场中的传播规律以及气体压力的变化开展研究。设计了直径20 mm、长度50、70、100 mm的3种不同尺寸药包,以尺寸控制液氧量,并设置了2个位置不同的压力传感器,对气体压力的变化进行全面的测量。通过选取气体传播过程中典型时刻的纹影图像分析气体前沿与混合气体的波动变化,对比分析3种液氧量下液氧相变膨胀的气体传播过程、速度变化、压力变化,并将理论分析与试验结果相结合,得到混合气体在自由场中传播规律及演化过程和压力分布特性。结果表明:从点火头引燃液氧吸收剂开始,液氧吸收剂释放出大量热量激发液氧迅速相变膨胀,气体在药包内部不断积累升温、升压,直至达到药包的致裂压力极限后,气体前沿与混合气体以药包为中心向外呈球形先伴随后分离式传播。液氧量增加,加速了液氧气化与能量聚集效率,分离时间随液氧量增大提前,累压时间由2.91 ms减少至1.20 ms,缩短了58.76%;气体前沿传播速度加快,速度峰值由1 025.64 m/s提升至1 487.18 m/s,增长了45%;测点1超压峰值压力由35.65 kPa增大到40.93 kPa,增长比例为14.57%;正压作用时间和峰值冲量的增长是非线性的,7 cm时均为最大,10 cm时均下降,药包过长可能导致相变能量分散或因长径比失衡引发湍流、反射波干扰,虽提升峰值压力但降低能量持续作用效率。

     

    Abstract: Aiming at the influence of different liquid oxygen filling volumes on the transient phase change expansion effect of liquid oxygen, the propagation laws of gas front and mixed gas generated by liquid oxygen phase change expansion in free field, as well as the variation characteristics of gas pressure, are investigated by using a high-speed schlieren system and an overpressure measurement system. Three charge cartridges with a diameter of 20 mm and lengths of 50 mm, 70 mm and 100 mm respectively are designed, the liquid oxygen filling volume is controlled by the cartridge size, and two pressure sensors arranged at different positions are adopted to realize comprehensive measurement of gas pressure variation. Schlieren images at typical moments during gas propagation are selected to analyze the wave variation of gas front and mixed gas, the gas propagation process, velocity variation and pressure variation during liquid oxygen phase change expansion under three liquid oxygen filling volumes are compared and analyzed, and the propagation laws, evolution processes and pressure distribution characteristics of mixed gas in free field are clarified by combining theoretical analysis with experimental results. Results show that, after the liquid oxygen absorbent is ignited by the ignition head, a large amount of heat is released by the absorbent to induce rapid phase change expansion of liquid oxygen. The gas is continuously accumulated, heated and pressurized inside the charge cartridge until the burst pressure limit of the cartridge is reached. After that, the gas front and mixed gas propagate outward in a spherical pattern with the cartridge as the center, presenting a mode of initial accompanying movement and subsequent separation. With the increase of liquid oxygen filling volume, the gasification and energy accumulation efficiency of liquid oxygen is improved, the separation time is advanced with the increase of liquid oxygen filling volume, and the pressure accumulation time is reduced from 2.91 ms to 1.20 ms, with a reduction rate of 58.76%. The propagation velocity of the gas front is increased, with the peak velocity rising from 1025.64 m/s to 1487.18 m/s, an increase rate of 45%. The peak overpressure at measuring point 1 is increased from 35.65 kPa to 40.93 kPa, with an increase rate of 14.57%. The positive pressure duration and peak impulse present a nonlinear growth trend, which reach the maximum at the cartridge length of 70 mm and decrease at the cartridge length of 100 mm. Excessively long charge cartridges may cause dispersion of phase change energy, or induce turbulence and reflected wave interference due to unbalanced length-to-diameter ratio. Although the peak overpressure can be increased under this condition, the continuous energy action efficiency is reduced.

     

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