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Magnetic field shielding of electromagnetic launch missile

机译:电磁发射导弹的磁场屏蔽

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Over the past three decades, electromagnetic launch technology has made significant progress. Some researchers have begun to study the missile which is accelerated by a railgun to supersonic speed. Compared to conventional missile, an electromagnetic launch missile has the advantages of high muzzle velocity and strong concealment. However, a railgun represents a harsh electromagnetic environment for the missile. Pulse current in the railgun can produce a high amplitude and broad spectrum magnetic field. Electromagnetic interference might affect any sensitive electrical devices that the missile is being equipped with. For this reason, it is necessary to study the missile magnetic field shield in rail launcher environment. This paper has built 3D model of the railgun and missile. Using finite-element analysis, we study separately missile inner magnetic field distribution under various shielding configurations, including monolayer shield-multilayer shield and the shield body with having hole. The shielding effectiveness (SE) of various shielding configurations is presented. Based on the above results, we design a kind of double layer shielding for missile in railgun. And this paper investigates the impact of the drilling point the hole size and the opening directions in shielding performance. In addition, we found that the electromagnetic force on the armature, namely, inductance gradient becomes large because of magnetic field shielding of missile. The relation between inductance gradient and shield has been analyzed. Study shows that inductance gradient is increased by 20%.
机译:在过去的三十年中,电磁发射技术取得了长足的进步。一些研究人员已经开始研究这种导弹,它是由一种轨道炮加速到超音速的。与常规导弹相比,电磁发射导弹具有较高的炮口速度和较强的隐蔽性。但是,电磁炮代表了导弹的恶劣电磁环境。轨道枪中的脉冲电流会产生高振幅和广谱的磁场。电磁干扰可能会影响导弹所配备的任何敏感电子设备。因此,有必要研究轨道发射器环境中的导弹磁场屏蔽。本文建立了电炮和导弹的3D模型。利用有限元分析,分别研究了单层屏蔽-多层屏蔽和带孔屏蔽体在各种屏蔽结构下的导弹内部磁场分布。介绍了各种屏蔽配置的屏蔽效果(SE)。基于以上结果,我们设计了一种用于轨道炮导弹的双层屏蔽。并研究了钻孔点的孔径和开孔方向对屏蔽性能的影响。另外,我们发现由于导弹的磁场屏蔽,电枢上的电磁力即电感梯度变大。分析了电感梯度与屏蔽之间的关系。研究表明,电感梯度增加了20%。

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