• Infrared and Laser Engineering
  • Vol. 51, Issue 4, 20210225 (2022)
Aiqiang Guo, Tianpeng Li, Xiaonan Li, and Xinbao Gao
Author Affiliations
  • Shijiazhuang Campus, Army Engineering University of PLA, Shijiazhuang 050003, China
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    DOI: 10.3788/IRLA20210225 Cite this Article
    Aiqiang Guo, Tianpeng Li, Xiaonan Li, Xinbao Gao. Simulation study of smoke screen jamming laser terminal guidance projectile[J]. Infrared and Laser Engineering, 2022, 51(4): 20210225 Copy Citation Text show less

    Abstract

    With the large-scale application of precision guided weapons, it has realized the transition from conventional ammunition cluster attack mode to guided munition precision strike mode, thus achieving the best combat cost performance. Its laser weapons are widely used in the military field to effectively combat laser weapons. Smoke screen bombs are favored by all countries due to their high cost-effective advantages. In this study, taking the smoke screen interferes with laser terminal guided projectiles as an example, the guidance principle of laser terminal guided projectiles, and the principle of smoke screen interference with laser terminal guided projectiles were studied. The shielding effect of the smoke screen on the laser seeker was introduced into the simulation process of external ballistic. Taking miss distance as an indicator, the jamming system simulation model was established, and the simulation research of smoke screen against laser terminal guided projectiles was realized. The research results show that the simulation system can provide the best jamming strategy for smoke screens against laser terminal guided projectiles, and can provide auxiliary decision-making for combat training and effectiveness evaluation of typical smoke munitions.
    ${P_d} = {E_d}/{\tau _d} \cdot {T_d}$(1)

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    ${P_t} = {P_d} \cdot {\tau _t}\left( {{R_{td}}} \right)$(2)

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    ${P_t} = {P_d}\dfrac{{\displaystyle\int_0^r {\exp } \left( { - \dfrac{{2{r^2}}}{{{w^2}}}} \right){\rm d}r}}{{\displaystyle\int_0^\infty {\exp } \left( { - \dfrac{{2{r^2}}}{{{w^2}}}} \right){\rm d}r}} \cdot {\tau _t}\left( {{R_{td}}} \right)$(3)

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    ${I_r} = {\rho _t}\dfrac{{{P_t}}}{{\pi R_{ts}^2}}\cos {\theta _L} \cdot {\tau _t}\left( {{R_{{{rs}}}}} \right)$(4)

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    $\cos {\theta _L} = \left| {\sin {\theta _d}\sin {\theta _s} + \cos {\theta _d}\cos {\theta _s}\cos \left( {{\varphi _d} - {\varphi _s}} \right)} \right|$(5)

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    ${C_{^Z}} = \dfrac{Q}{{\sqrt {\pi /2} u{\sigma _y}}}\exp \left( { - \dfrac{{{y^2}}}{{2\sigma _y^2}}} \right)$(6)

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    ${\tau _t}(L) = {\tau _{ab}}(L) \cdot {\tau _{sc}}(L)$(7)

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    ${\tau _{ab}}\left( L \right) = 1 - ERF\left( {0.0167\sqrt W } \right)$(8)

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    ${\tau _{sc}}\left( L \right) = {\tau _1}\left( L \right){\tau _2}\left( L \right){\tau _3}\left( L \right)$(9)

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    ${\tau _1}(L) = {{\rm e}^{ - \gamma (1.06)t}}$(10)

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    $\gamma (1.06) = \dfrac{{3.912}}{{{R_v}}}{(1.93)^{ - q}}$(11)

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    $q = \left\{ {\begin{array}{l} {1.3,\;{\kern 1pt} {R_v} \geqslant 11\; {\rm km}} \\ {0.585R_v^{1/3},\;{R_v} < 11\;{\rm km}} \end{array}} \right.$(12)

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    ${\tau _2}(L) = {{\rm e}^{ - \frac{{3.912}}{{{R_v}}}L}}$(13)

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    ${r_1}(L) = {{\rm e}^{ - \delta L}}$(14)

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    Aiqiang Guo, Tianpeng Li, Xiaonan Li, Xinbao Gao. Simulation study of smoke screen jamming laser terminal guidance projectile[J]. Infrared and Laser Engineering, 2022, 51(4): 20210225
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