含炭吸收剂的液氧瞬态相变膨胀气体传播规律及强度特性研究

Propagation and intensity characteristics of expansion gases from transient phase change of liquid oxygen with carbon-containing absorbents

  • 摘要: 针对不同含炭量吸收剂对液氧瞬态相变膨胀效果的影响问题,设计了含炭量分别为0、0.1、0.2 g的3种液氧药包,借助高速纹影系统与超压测量系统对液氧瞬态相变膨胀产生的气体前驱和相变产物在纹影流场中的传播规律以及相变气体压力的强度变化开展对比分析,并将理论分析与实验结果相结合,得到相变气体在空气流场中传播规律及演化过程和压力分布特性。研究结果表明:①含炭量对相变膨胀特性调控显著,随着含炭量从0增至0.2 g,起爆时间从1.32 ms延长至3.69 ms,累压时间增加180%;②气体前驱传播速度大幅提升,水平方向最大速度从473.96 m/s提升至692.71 m/s,垂直方向最大速度从875.00 m/s增至1 604.17 m/s;③超压峰值呈非线性增长,轴向超压从7.754 MPa增至16.567 MPa,径向从1.301 MPa增至4.838 MPa;④气体前驱与相变产物分离时间从60 μs延长至110 μs,垂直方向位移普遍大于水平方向,呈现“上下快、左右慢”的各向异性传播特征。

     

    Abstract: This study investigates how different carbon-containing absorbents affect the transient phase change expansion of liquid oxygen. Specifically, we prepared 3 types of liquid oxygen charges with varying carbon contents (0, 0.1 g, and 0.2 g). A high-speed schlieren system and an overpressure measurement system were used for comparative analysis on the propagation patterns of gas precursor and phase change products in the schlieren flow field and the intensity changes of the phase change gas pressure. Both theoretical and experimental analysis were conducted to unveil the propagation patterns, evolution process and pressure distribution of the phase change gas in the air flow field. Results show that ① Carbon content exerts a significant regulatory effect on phase change expansion. As the carbon content increased from 0 to 0.2 g, the initiation time increased from 1.32 ms to 3.69 ms, and the cumulative pressure time increased by 180 %. ② The propagation speed of the gas precursor exhibited significant increase, with maximum horizontal speed rising from 473.96 m/s to 692.71 m/s and vertical speed from 875.00 m/s to 1 604.17 m/s. ③ Peak overpressure showed nonlinear growth, with axial overpressure increasing from 7.754 MPa to 16.567 MPa and radial overpressure from 1.301 MPa to 4.838 MPa. ④ Separation time between the gas precursor and the phase change products increased from 60 μs to 110 μs. Vertical displacement generally exceeded horizontal displacement, showing an anisotropic propagation pattern of "rapid vertical expansion and slow lateral spread".

     

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