{"title":"Comparison of Railguns through Numerical Simulations","authors":"W. Yuan, P. Yan","doi":"10.1109/ELT.2008.22","DOIUrl":null,"url":null,"abstract":"Up to date, the armature transition is still a big problem in railgunnery. Many kinds of mechanism were proposed by researchers to predict or explain armature transition phenomena. And many types of railgun were invented. In this paper, three types of railgun, including simple railgun, parallel-augmented railgun and muzzle-fed railgun, are investigated with numerical simulations. Since current density is the decisive factor to transition velocity, this study focuses on the current distribution in armature. The inductance gradient of railgun and magnetic field distribution are also investigated. In order to simplify simulations, rails and armature are considered in each simulation, and armatures of railgun are same. The Maxwell 3D modular of Ansoft corp. was utilized as the program code. The simple railgun is selected as the benchmark, and the other two types were compared with it. In the simulation of parallel-augmented railgun, two current sources (500 kA, 60 Hz) were connected to inner rails and outer rail independently. In muzzle-fed railgun simulation, the same current source as in simple railgun was connected to rails. Based on simulation results, conclusions are drawn that augmented railgun has the highest inductance gradient and the largest launcher efficiency. But the current density at rear part of armature is larger than that of simple railgun if the currents flowing through inner rails and outer rail are equal. The inductance gradient of muzzle-fed railgun is the smallest, but the current density at armature shoulder is the largest. Projectiles of muzzle-fed railgun will face the greatest magnetic flux density.","PeriodicalId":170049,"journal":{"name":"2008 14th Symposium on Electromagnetic Launch Technology","volume":"160 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-06-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2008 14th Symposium on Electromagnetic Launch Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ELT.2008.22","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 2
Abstract
Up to date, the armature transition is still a big problem in railgunnery. Many kinds of mechanism were proposed by researchers to predict or explain armature transition phenomena. And many types of railgun were invented. In this paper, three types of railgun, including simple railgun, parallel-augmented railgun and muzzle-fed railgun, are investigated with numerical simulations. Since current density is the decisive factor to transition velocity, this study focuses on the current distribution in armature. The inductance gradient of railgun and magnetic field distribution are also investigated. In order to simplify simulations, rails and armature are considered in each simulation, and armatures of railgun are same. The Maxwell 3D modular of Ansoft corp. was utilized as the program code. The simple railgun is selected as the benchmark, and the other two types were compared with it. In the simulation of parallel-augmented railgun, two current sources (500 kA, 60 Hz) were connected to inner rails and outer rail independently. In muzzle-fed railgun simulation, the same current source as in simple railgun was connected to rails. Based on simulation results, conclusions are drawn that augmented railgun has the highest inductance gradient and the largest launcher efficiency. But the current density at rear part of armature is larger than that of simple railgun if the currents flowing through inner rails and outer rail are equal. The inductance gradient of muzzle-fed railgun is the smallest, but the current density at armature shoulder is the largest. Projectiles of muzzle-fed railgun will face the greatest magnetic flux density.
迄今为止,电枢转换仍然是轨道炮中的一个大问题。研究者们提出了多种机制来预测或解释电枢过渡现象。许多类型的轨道炮被发明出来。本文对简单轨道炮、平行增强型轨道炮和前膛式轨道炮三种类型的轨道炮进行了数值模拟研究。由于电流密度是影响过渡速度的决定性因素,因此本文主要研究电枢内的电流分布。研究了轨道炮的电感梯度和磁场分布。为了简化仿真,每次仿真都考虑轨道和电枢,轨道炮的电枢是相同的。程序代码采用安软公司的Maxwell 3D模块。选择简单轨道炮作为基准,并与其他两种类型进行了比较。在并联增强型轨道炮仿真中,分别将两个电流源(500 kA, 60 Hz)分别连接到内轨和外轨。在膛控轨道炮仿真中,将与简单轨道炮相同的电流源连接到轨道上。仿真结果表明,增强型轨道炮具有最大的电感梯度和最大的发射效率。但在通过内轨和外轨的电流相等的情况下,电枢后部的电流密度比简单的轨道炮大。轨道炮的电感梯度最小,但电枢肩处的电流密度最大。轨道炮的弹丸将面临最大的磁通密度。