nav emailalert searchbtn searchbox tablepage yinyongbenwen piczone journalimg journalInfo journalinfonormal searchdiv searchzone qikanlogo popupnotification paper paperNew
2026, 01, v.47 70-79
含包覆药的混合装药二维两相流内弹道仿真研究
基金项目(Foundation):
邮箱(Email):
DOI: 10.19323/j.issn.1673-6524.202407007
摘要:

针对大口径火炮含包覆药的混合装药内弹道问题,建立了含包覆药的混合装药二维两相流内弹道数学模型,并利用该模型开展了某大口径火炮含包覆药的混合装药内弹道过程以及单一装药内弹道过程的对比研究,并探讨了包覆发射药质量占比和包覆层质量分数对内弹道性能的影响。结果表明,与未包覆、单一装药内弹道性能相比,在保证相同弹丸初速条件下,含包覆药的混合装药能够将最大膛压由336.9 MPa下降至318.6 MPa。当包覆发射药质量占比由0增大至30%和70%时,炮口动能分别低了7%和17%,而最大膛压分别降低了18%和39%。当包覆层质量分数占比由2.5%增大至7.5%和12.5%时,炮口动能分别低了3%和5%,而最大膛压分别降低了7%和14%。

Abstract:

Aiming at solving the interior ballistic problem of a large caliber cannon which used mixed charge with coated propellant, a two-dimensional two-phase flow interior ballistic model of mixed charge with coated propellant was established. Based on this model, the interior ballistic processes of mixed charge with coated propellant were compared with those of uncoated single charge, and the influe-nce of the mass ratio of coated charge and the coating layer mass fraction on interior ballistics perfor-mance was investigated. The results showed that compared with the interior ballistics performance of uncoated single charge, the the coated mixed charge could reduce the maximum chamber pressure from 336.9 MPa into 318.6 MPa at the same muzzle velocity. When the mass ratio of coated charge was increased from 0 to 30% and 70%, the muzzle energy was decreased by 7% and 17% respectively, and the maximum chamber pressure was reduced by 18% and 39% respectively. When the coating layer mass fraction was increased from 2.5% to 7.5% and 12.5%, the muzzle energy was reduced by 3% and 5% respectively, and the maximum chamber pressure was reduced by 7% and 14% respectively.

参考文献

[1] 尹记红.某105 mm高膛压火炮包覆混合装药双一维两相流数值仿真[D].南京:南京理工大学,2021.

[2] SIKDER A K,REDDY S T.Review on energetic thermoplastic elastomers (ETPEs) for military science[J].Propellants,Explosives,Pyrotechnics,2013,38(1):14-28.

[3] 徐前.包覆混合装药的定容燃烧性能研究[D].南京:南京理工大学,2016.

[4] 徐前,何卫东.横切棒状和包覆粒状发射药混合装药定容燃烧性能[J].含能材料,2017,25(1):39-43.

[5] 魏伦,于慧芳,韩冰,等.一种新型聚酯钝感剂在发射药中的应用[J].火炸药学报,2012,35(3):91-94.

[6] DAHIWALE S,BHONGALE C J,ROY S,et al.Studies on the ballistic parameters of a deterred triple base propellant used in large caliber ammunition[J].Central Euro-pean Journalof Energetic Materials,2019,16(3):449-467.

[7] 刘志涛,徐滨,南风强,等.低温感包覆火药燃烧过程破孔规律研究[J].南京理工大学学报,2011,35(5):709-713.

[8] 许涛.部分切口杆状药、包覆药及其混合装药渐增性燃烧性能研究[D].南京:南京理工大学,2016.

[9] 张丽娜,王英博,南风强,等.双层包覆对超多孔发射药燃烧性能的影响[J].含能材料,2020,28(6):498-503.

[10] 沈万武.超多孔发射药包覆工艺及燃烧性能研究[D].南京:南京理工大学,2019.

[11] 王琳.125 mm穿甲弹装药设计优化探索研究[D].南京:南京理工大学,2007.

[12] 宋时育,王泽山.低温感发射装药弹道性能的研究[J].火炸药学报,2000(2):4-7.

[13] 史先扬,王泽山.低温感硝胺火药定容燃烧特性研究[J].火炸药学报,2002(3):61-63.

[14] 豆松松,狄加伟,聂奎,等.采用包覆随行装药提高炮射导弹内弹道性能的数值预测[J].火炮发射与控制学报,2019,40(1):84-88.

[15] 程申申,王浩,薛绍,等.基于五阶WENO格式的燃气在药床中流动过程二维两相流研究[J].爆炸与冲击,2021,41(6):062902.

[16] 肖辉鹏,王浩,陶如意.基于OpenFOAM的三维内弹道两相流程序开发及其应用[J].弹道学报,2020,32(1):64-70.

[17] 程诚,张小兵.内弹道两相流三维并行数值模拟[J].兵工学报,2019,40(4):769-776.

[18] 马天一,陶如意,森思义,等.单模块装药膛内流场特性试验及数值仿真[J].含能材料,2023,31(1):70-82.

[19] 马天一,陶如意,周思渊,等.模块装药短管炮实验及数值模拟研究[J].弹道学报,2024,36(2):44-52.

[20] 刘子豪.点传火射流两相流动及点火燃气在模块药盒内传播特性研究[D].南京:南京理工大学,2019:9-21.

[21] 周彦煌,王升晨.实用两相流内弹道学[M].北京:兵器工业出版社,1990:278-283.

[22] 白桥栋.CE/SE方法在内弹道两相流中应用的研究[D].南京:南京理工大学,2007:41-58.

基本信息:

DOI:10.19323/j.issn.1673-6524.202407007

中图分类号:TJ301

引用信息:

[1]冯渊,王育维,朱文芳,等.含包覆药的混合装药二维两相流内弹道仿真研究[J].火炮发射与控制学报,2026,47(01):70-79.DOI:10.19323/j.issn.1673-6524.202407007.

检 索 高级检索

引用

GB/T 7714-2015 格式引文
MLA格式引文
APA格式引文