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Imploding Foil Liner Experiments on the MIG Pulse Generator

机译:MIG脉冲发生器的内爆箔衬板实验

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The energy density in the plasma column formed during the implosion of a cylindrical liner by the current of a powerful generator is largely determined by the radius of the liner. When the liner is accelerated to a given velocity, the liner's initial radius is proportional to the rise time of the generator current. With a current rise time of ∼ 100 ns and a liner velocity of $sim 3imes 10^{7} ext{cm}/mathrm{s}$ (before stagnation), it is necessary to choose a liner radius of about 1 cm. The paper presents experiments on imploding foil liners with a diameter of 1-2 mm when the current front through the liner is sharpened to several nanoseconds. In particular, upon implosion of a 1-mm-diameter liner from $2.5-mu mathrm{m}$-thick aluminum foil with a current of about 2 MA, a column of plasma with a diameter of not more than $70 mu mathrm{m}$ was obtained. An estimate of the energy density in the plasma column gives $geq 1.5imes 10^{8} mathrm{J}/ext{cm}^{3}$.
机译:在由强力发生器的电流将圆柱形衬套内爆期间形成的等离子柱中的能量密度在很大程度上取决于衬套的半径。当衬套加速到给定速度时,衬套的初始半径与发电机电流的上升时间成比例。电流上升时间约为100 ns,线性速度为 $ sim 3 \ times 10 ^ {7} \ \ text {cm} / \ mathrm {s} $ (在停滞之前),有必要选择大约1厘米的衬管半径。本文介绍了在通过衬套的电流前沿锐化至几纳秒时对直径为1-2 mm的内爆箔衬套进行的实验。特别是在爆破直径为1毫米的衬管时 $ 2.5- \ mu \ mathrm { m} $ 电流约为2 MA的厚铝箔,等离子柱直径不大于 $ 70 \ \ mu \ mathrm { m} $ 获得了。对等离子柱中能量密度的估算得出 $ \ geq 1.5 \ times 10 ^ {8} \ \ mathrm {J} / \ text {cm} ^ {3} $

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