环形双锥罩聚能装药结构优化设计

刘宏杰; 王伟力; 苗润; 吴世永

doi:10.11858/gywlxb.20180539

环形双锥罩聚能装药结构优化设计

doi: 10.11858/gywlxb.20180539

刘宏杰^1,,
王伟力^2,*, ,,
苗润¹,
吴世永³

1.
海军航空大学岸防兵学院, 山东烟台 264001
2.
海军工程大学兵器工程学院, 湖北武汉 432032
3.
海军航空大学基础部, 山东烟台 264001

详细信息

作者简介:
刘宏杰(1993-), 男, 硕士研究生, 主要从事弹药设计与目标毁伤评估研究. E-mail:1300202650@qq.com

通讯作者:
王伟力(1962—)，男，教授，博士生导师，主要从事战斗部毁伤效应研究. E-mail:wwl85673@163.com

中图分类号: TJ410.3
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出版历程
- 收稿日期: 2018-04-19
- 修回日期: 2018-05-30

Optimum Design of Annular Double Done Shaped Charge Structure

LIU Hongjie^1
,,
WANG Weili^{2,*
, ,},
MIAO Run¹,
WU Shiyong³

1.
Coastal Defense College, Naval Aeronautical University, Yantai 264001, China
2.
Academy of Weapons Engineering, Naval Engineering University, Wuhan 432032, China
3.
Basic Department, Naval Aeronautical University, Yantai 264001, China

摘要

摘要: 在环形聚能装药结构中，单锥罩结构形成的射流中间有堆积现象，断裂前射流拉伸长度有限，而双锥罩射流兼顾了上锥小锥角形成高头部速度，下锥大锥角增大射流有效质量的优点，形成的射流更加细长，头部速度高且不易断裂。基于环形切割聚能装药战斗部，综合考虑上锥角大小、上锥罩占药型罩高的比例、药型罩的高度以及药型罩壁厚对射流侵彻能力的影响，并基于灰关联理论对双锥罩环形聚能装药的优化提供依据，通过数值仿真，研究表明：上下锥角对射流成型影响最大，通过比较，当上锥罩为34°、上锥占罩高比例为40%、药型罩高度为70 mm、药型罩壁厚为5 mm时，形成的射流头部速度高，且在空气中能够稳定飞行。相比单锥罩结构，双锥罩射流细长，在空气中飞行时间长，对靶板的侵深大于单锥罩射流。
- 串联战斗部 /
- 环形双锥罩 /
- 正交设计 /
- 数值模拟
Abstract: There is accumulation in the middle of the jets formed by the single cone liner in the annular shaped charge structure, and the length of the jet is limited before the fracture.The jet of the double cone liner takes both the high head speed formed by upper small angle cone liner and increscent effective mass of the jet formed by the lower cone liner.Therefore, the jet is more slender with high head speed and it is not easy to break.Based on the annular cutting shaped charge warhead, the influence of the upper cone size, the proportion of the upper cone cover, the mask height and the wall thickness of the liner on the penetration capability of jet is considered.It is concluded that the upper cone angle has the greatest influence on the jet molding.By comparison, when the top cone cover is 34°, the proportion of top cone is 40%, the height of the liner is 70 mm and the wall thickness of the liner is 5 mm, the jet head can fly steadily in the air with a high speed.Compared with the single cone liner structure, the jet formed by the double cone liner is long and slender, and has long flight time in the air, its penetration capability is greater than that of the single cone jet.
- tandem warhead /
- annular double cone liner /
- orthogonal design /
- numerical simulation

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图 1 装药结构示意图

Figure 1. Schematic structure of shaped charge

下载: 全尺寸图片幻灯片

图 2 双锥罩射流成型参数随上锥角的变化曲线

Figure 2. Variation of double cone liner jet parameters with the upper cone angle

下载: 全尺寸图片幻灯片

图 3 双锥罩射流成型参数随壁厚的变化曲线

Figure 3. Variation of double cone liner jet parameters with the thickness of liner

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图 4 双锥罩射流成型参数随药型罩高度的变化曲线

Figure 4. Variation of double cone liner jet parameters with the height of the liner

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图 5 双锥罩射流成型参数随上锥罩占罩高比例的变化曲线

Figure 5. Variation of double cone liner jet parameters with the proportion of the upper cone cover

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图 6 双锥罩射流成型图

Figure 6. Forming of double cone liner jet

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图 7 单锥罩射流成型图

Figure 7. Forming of single cone liner jet

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图 8 两种射流侵彻靶板结果图

Figure 8. Result diagrams of two kinds of jet penetrating target plate

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表 1 B炸药计算参数

Table 1. Material performance parameters of composition B

ρ/(g·cm^-3)	D/(m·s^-1)	p_CJ/GPa	A/GPa	B/GPa	R₁	R₂	ω	E₀/GPa	V₀
1.713	7500	28.6	524.2	7.678	4.2	1.1	0.34	8.499	1.0

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表 2 药型罩计算参数^[13]

Table 2. Material performance parameters of liner^[13]

ρ/(g·cm^-3)	G₀/GPa	σ₀/GPa	T_m0/K	C/(m·s^-1)	S₁	A	β	n	a
8.96	47.7	0.12	1790	3940	1.49	63.5	36	0.45	1.5

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表 3 30CrMnSiNi2A计算参数

Table 3. Material performance parameters of 30CrMnSiNi2A

A/MPa	B/MPa	n	C	m	T_m/K	T₀/K	S₁	γ₀	α
1280	420	0.30	0.03	1.00	1793	294	1.49	2.17	0.46

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表 4 钢板计算参数^[16]

Table 4. Material performance parameters of steel plate^[16]

ρ/(g·cm^-3)	E/GPa	μ	σ_s/MPa
7.85	207	0.30	600

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表 5 空气的计算参数

Table 5. Material performance parameters of air

ρ/(mg·cm^-3)	C₄	C₅	E₀/(MJ·m^-3)	v_rel
1.293	0.4	0.4	0.25	1.0

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表 6 正交设计各因子水平值

Table 6. Orthogonal table

Level	α/(°)	b₁/mm	H/mm	h·H^-1/%
1	30	3.8	60	30
2	36	4.6	70	50
3	44	5.4	80	70

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表 7 正交表设计与计算结果

Table 7. Orthogonal design and calculation result

No.	α/(°)	b₁/mm	H/mm	h·H^-1/%	V/(m·s^-1)	L/mm
1	30	3.8	60	30	2807	25
2	30	4.6	70	50	2469	70
3	30	5.4	80	70	2488	70
4	36	3.8	70	70	2297	45
5	36	4.6	80	30	2804	70
6	36	5.4	60	50	2871	90
7	44	3.8	80	30	2834	40
8	44	4.6	60	70	2470	55
9	44	5.4	70	50	2508	70

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表 8 无量纲化的参考序列与比较序列

Table 8. Dimensionless reference sequence and comparison sequence

No.	X₁^′	X₂^′	X₃^′	X₄^′	Y₁^′	Y₂^′
1	1	1	1	1	1	1
2	1	1.211	1.1667	1.6667	0.8796	2.8
3	1	1.421	1.3333	2.3333	0.8864	2.8
4	1.2	1	1.1667	2.3333	0.8183	1.8
5	1.2	1.211	1.3333	1	1.0003	2.8
6	1.2	1.421	1	1.6667	1.0228	3.6
7	1.467	1	1.3333	1	1.0096	1.6
8	1.467	1.211	1	2.3333	0.8799	2.2
9	1.467	1.421	1.1667	1.6667	0.8935	2.8

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表 9 灰关联度矩阵

Table 9. Grey correlation matrix

Reference sequence	Comparison sequence
Reference sequence	α	b₁	H	h·H^-1
V₁	0.528	0.475	0.554	0.373
L	0.740	0.714	0.755	0.579

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