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活性内芯侵爆结构侵彻多层间隔靶自分布释能机理与模型研究

向镜安1,王海福1,闫月光1,曲利峰2,葛超1*   

  1. 1.北京理工大学 爆炸科学与安全防护全国重点实验室;2.陆装驻成都地区第三军代室,陆装驻成都地区第三军代室
  • 收稿日期:2024-09-20 修回日期:2024-12-05
  • 基金资助:
    国家自然科学基金项目(12302460);爆炸科学与安全防护全国重点实验室基金项目(YBKT24-02)

Mechanism and Theoretical Model of Self-Distributed Energy Release Behavior on Reactive Filling Structure Penetrating Multi-Layered Plates

XIANG Jing’an1,WANG Haifu1,YAN Yueguang1,QU Lifeng2 GE Chao1*   

  1. 1. State Key Laboratory of Explosion Science and Safety Protection, Beijing Institute of Technology; 2.PLA in Chengdu Area of the Third Military Office
  • Received:2024-09-20 Revised:2024-12-05

摘要: 活性内芯侵爆结构作用多层目标展现独特的自分布爆燃释能、力化耦合时空穿爆特性,在靶后空间形成多峰值、长持续爆燃反应超压,爆燃反应演化行为与靶后超压形成机理复杂。针对这种独特的释能行为,开展不同速度侵爆结构侵彻间隔结构靶试验,建立描述活性内芯靶后空间爆燃行为的等效爆燃点模型与活性材料爆燃超压模型,揭示侵爆结构侵彻多层间隔靶后自由场超压特性形成机理。研究结果表明:侵爆结构以594~819 m/s碰撞结构靶,产生对应范围为2.54~3.92 GPa的碰撞应力,均在第三层靶板出现最大超压峰值,超压峰值随碰撞速度增加从0.0607 MPa增加至0.246 MPa;依据等效爆燃点模型,侵爆结构在靶后20.73 mm距离内发生剧烈爆燃反应;侵爆结构头部厚度、碰撞速度、靶板厚度等参数通过影响有效激活芯体质量耦合影响爆燃超压峰值。通过对比试验数据与拟合模型,验证了活性材料爆燃超压模型准确性,为侵爆结构后效毁伤研究提供支撑。

关键词: 活性内芯侵爆结构, 靶后超压, 活性材料, 多层结构靶

Abstract: The reactive filling structure exhibits a unique behavior of self-distributed deflagration and energy release, along with mechanically and chemically coupled dynamic characteristics when penetrating multi-layered plates. This results in a multi-peak, long-duration deflagration overpressure behind the plates, featuring a complex evolution and waveform mechanism of the deflagration process. To better understand this distinctive energy-releasing behavior, overpressure signals were recorded during experiments that involved the reactive filling structure penetrating multi-layered plates at various velocities. An equivalent deflagration position model and theories for deflagration overpressure were developed to clarify the waveform characteristics of deflagration shock wave. Experimental results show that the third collision produced the maximum peak overpressure., which increased from 0.0607 MPa to 0.246 MPa as the velocity rose from 594 m/s to 819 m/s(the impact stress in the range of 2.54 GPa to 3.92 GPa). The equivalent deflagration model indicates that the intense deflagration reaction occurred within a distance of 20.73 mm behind the plates. The peak deflagration overpressure is influenced by several factors, including thickness of the structure's head, the impact velocity, and the thickness of plates, all of which affect the effective initiated mass of the reactive filling. The analytical model aligns well with the experimental results, providing credible support for further investigations into the after-effects of the reactive filling structure.

Key words: reactive filling structure, behind-plate overpressure, reactive materials, multi-layered plates

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