• Acta Physica Sinica
  • Vol. 68, Issue 7, 070601-1 (2019)
Bing-Ting Zha1、2、*, Hai-Lu Yuan1, Shao-Jie Ma1、2, and Guang-Song Chen1、2
Author Affiliations
  • 1Key Discipline Laboratory of Intelligent Ammunition Technology National Defense, Nanjing University of Science and Technology, Nanjing 210094, China
  • 2Changshu Research Institute Co.Ltd, Nanjing University of Science and Technology, Changshu 215513, China
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    DOI: 10.7498/aps.68.20181860 Cite this Article
    Bing-Ting Zha, Hai-Lu Yuan, Shao-Jie Ma, Guang-Song Chen. Influence of single-beam expanding scanning laser circumferential detection system parameters on detection capability[J]. Acta Physica Sinica, 2019, 68(7): 070601-1 Copy Citation Text show less
    The structure of a single beam expanding beam scanning laser periscope detection system.单光束扩束扫描激光周视探测系统结构
    Fig. 1. The structure of a single beam expanding beam scanning laser periscope detection system.单光束扩束扫描激光周视探测系统结构
    Schematic diagram of detection target of single-beam pulsed laser circumferential scan detection system.单光束脉冲激光周向扫描探测系统探测目标示意图[11]
    Fig. 2. Schematic diagram of detection target of single-beam pulsed laser circumferential scan detection system.单光束脉冲激光周向扫描探测系统探测目标示意图[11]
    Pulse beam view in the positive direction of the x-axis.沿x轴正方向脉冲光束视图
    Fig. 3. Pulse beam view in the positive direction of the x-axis. 沿x轴正方向脉冲光束视图
    Projection of adjacent pulsed laser beam on plane M.相邻脉冲激光束在面M上的投影
    Fig. 4. Projection of adjacent pulsed laser beam on plane M. 相邻脉冲激光束在面M上的投影
    Geometrical relationship between the laser beam and the projected image.发射激光束与投影图像几何关系
    Fig. 5. Geometrical relationship between the laser beam and the projected image.发射激光束与投影图像几何关系
    The echo power with different K(R), R and : (a) ; (b) ; (c) 回波功率Pr与K(R), R, 之间的关系 (a) ; (b) ; (c)
    Fig. 6. The echo power with different K(R), R and : (a) ; (b) ; (c) 回波功率PrK(R), R, 之间的关系 (a) ; (b) ; (c)
    Mathematical model of K(R): (a) The position of the center line of the beam; (b) the K(R) model when the left side of the beam intersects the target; (c) the K(R) model when the left side of the beam is separated from the target.K(R)数学模型 (a)光束中心线位置示意图; (b)光束左边沿线与目标相交时K(R)模型; (c)光束左边沿线与目标相离时K(R)模型
    Fig. 7. Mathematical model of K(R): (a) The position of the center line of the beam; (b) the K(R) model when the left side of the beam intersects the target; (c) the K(R) model when the left side of the beam is separated from the target. K(R)数学模型 (a)光束中心线位置示意图; (b)光束左边沿线与目标相交时K(R)模型; (c)光束左边沿线与目标相离时K(R)模型
    The relationship between K(R) and , and : (a) The relationship between K(R) and , ; (b) the influence curve of , and on K(R).K(R)与, 和之间的关系 (a) , 与K(R)的关系; (b) , 和对K(R)的影响曲线
    Fig. 8. The relationship between K(R) and , and : (a) The relationship between K(R) and , ; (b) the influence curve of , and on K(R). K(R)与 , 和 之间的关系 (a) , 与K(R)的关系; (b) , 和 对K(R)的影响曲线
    Effects of pulse frequency f, beam angle , and beam incidence angle on targets with different diameters: (a) ; (b) ; (c) .脉冲频率f、光束角和光束入射角对不同目标直径的影响 (a) ; (b) ; (c)
    Fig. 9. Effects of pulse frequency f, beam angle , and beam incidence angle on targets with different diameters: (a) ; (b) ; (c) . 脉冲频率f、光束角 和光束入射角 对不同目标直径的影响 (a) ; (b) ; (c)
    Maximum angle between adjacent pulse beams: (a) The relation curve between f1 and the position of the target circle; (b) value of and .最大相邻脉冲光束夹角(a) f1与目标圆位置关系曲线; (b) 与取值计算
    Fig. 10. Maximum angle between adjacent pulse beams: (a) The relation curve between f1 and the position of the target circle; (b) value of and . 最大相邻脉冲光束夹角  (a) f1与目标圆位置关系曲线; (b) 与 取值计算
    Influence of and on echo power. (a) ; (b) ; (c) .和对系统回波功率的影响 (a) ; (b) ; (c)
    Fig. 11. Influence of and on echo power. (a) ; (b) ; (c) . 和 对系统回波功率的影响 (a) ; (b) ; (c)
    ParameterValueParameterValue
    Pt/W 70Pmin/ ${\text{μ}}$W 5
    vm/m·s–1700vt/m·s–1200
    Lt/m 3$\eta$0.9
    Ar/m20.00031$\sigma$/m–10.00054
    $\theta_{\simfont\text{边界}}$/rad 0.26$\xi_{\simfont\text{边界}}$/rad ${\text{π}}/2$
    Table 1.

    Simulation parameters of the detection system.

    探测系统仿真参数

    ParameterValueParameterValue
    Pt/W 70Dt/m 0.18
    R/m 6${\alpha _{\rm{t}}}$${\text{π}}/3$, ${\text{π}}/4$, ${\text{π}}/6$
    Table 2.

    Calculate the minimum pulse frequency and beam angle system parameters

    计算最低脉冲频率及光束角系统参数

    入射角扩束前扩束后
    ${\alpha _{\rm{t}}}$/rad $\xi$/rad $\theta$/rad kf/Hz ${\xi _{\max}}$/rad ${\theta _{\max }}$/rad kminfmin/Hz
    ${\text{π}}/3$0.03450.0025182544110.24170.2417267798.74
    ${\text{π}}/4$0.04220.0025149444250.25130.2513257500.82
    ${\text{π}}/6$0.05980.0025105314110.25130.2513257500.82
    Table 3. nmin, , and fmin at different incident angles . 不同入射角 下的nmin, , 以及fmin
    Bing-Ting Zha, Hai-Lu Yuan, Shao-Jie Ma, Guang-Song Chen. Influence of single-beam expanding scanning laser circumferential detection system parameters on detection capability[J]. Acta Physica Sinica, 2019, 68(7): 070601-1
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