Vcr=2EIkρA, ]]> where E is Young's modulus for the rail, I is moment of inertia for the rail, k is foundation modulus for the support, ρ is density for the rail and A is the cross-sectional area of the rail. The launcher is configured such that the critical velocity increases along the axial direction towards the muzzle. In particular, a material term √E/ρ of the rail increases along the axial direction, such for the rail being made from a first material being proximate to the breech and a second material being proximate to the muzzle, such that the material term √E/ρ of the second material being greater than that of the first material. Alternatively, the rail is made into a first shape being proximate to the breech and a second shape being proximate to the muzzle, such that a shape term √I/A of the second shape is greater than that of the first shape."/> Rails for electromagnetic hypervelocity launcher
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Rails for electromagnetic hypervelocity launcher

机译:电磁超高速发射器的导轨

摘要

An electromagnetic launcher is provided for accelerating a projectile from a breech end to a muzzle end. The launcher includes a container, a rail contained therein and a support. The container includes an inner surface along an axial direction. The rail is contained within the inner surface and includes a load surface to support the projectile and an interface surface. The support is disposed between the interface surface and the inner surface. The rail and the support provide a value to an expression for critical velocity; <math overflow="scroll"><mrow><mrow><msub><mi>V</mi><mi>cr</mi></msub><mo>=</mo><msqrt><mfrac><mrow><mn>2</mn><mo>⁢</mo><msqrt><mi>EIk</mi></msqrt></mrow><mrow><mi>ρ</mi><mo>⁢</mo><mstyle><mspace width="0.3em" height="0.3ex" /></mstyle><mo>⁢</mo><mi>A</mi></mrow></mfrac></msqrt></mrow><mo>,</mo></mrow></math> where E is Young's modulus for the rail, I is moment of inertia for the rail, k is foundation modulus for the support, ρ is density for the rail and A is the cross-sectional area of the rail. The launcher is configured such that the critical velocity increases along the axial direction towards the muzzle. In particular, a material term √E/ρ of the rail increases along the axial direction, such for the rail being made from a first material being proximate to the breech and a second material being proximate to the muzzle, such that the material term √E/ρ of the second material being greater than that of the first material. Alternatively, the rail is made into a first shape being proximate to the breech and a second shape being proximate to the muzzle, such that a shape term √I/A of the second shape is greater than that of the first shape.
机译:提供了一种电磁发射器,用于将弹丸从后膛端加速到枪口端。发射器包括容器,容纳在其中的轨道和支撑件。容器包括沿轴向的内表面。轨道被包含在内表面内并且包括支撑弹丸的载荷表面和界面。支撑件设置在界面和内表面之间。轨道和支撑为临界速度的表达式提供了价值。 <![CDATA [<数学溢出=“ scroll”> V cr = < / mo> 2 EIk ρ A ]]> 其中E是轨道的杨氏模量,I是轨道的惯性矩,k是支撑的基础模量,ρ是轨道的密度,A是轨道的横截面积。发射器构造成使得临界速度沿着轴向朝向枪口增大。特别地,轨道的材料项√E/ρ沿着轴向方向增加,使得轨道由靠近后膛的第一材料和靠近枪口的第二材料制成,使得材料项√第二材料的E /ρ大于第一材料的E /ρ。替代地,将轨道制成靠近后膛的第一形状和靠近枪口的第二形状,使得第二形状的形状项√I/ A大于第一形状的形状项。

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