正电射线。

J. ThomsonJ.
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引用次数: 247

摘要

1886年,戈尔茨坦观察到,当真空管中的阴极被穿孔时,放电不会在阴极停止;在阴极后面,可以看到光束以图1所示的方式流过孔。他把这些铅笔状的光归因于穿过孔进入阴极后面气体的光线;根据它们与通过阴极的通道的联系,他称这些射线为卡纳斯特拉伦。阴极后面的光的颜色取决于管里的气体:有空气的光是淡黄色的,有氢气的光是玫瑰色的,有霓虹灯的光是绚丽的霓虹灯红色,这种气体的效果非常惊人。当光线照射到管壁上时,会产生磷光;它们也会影响照相底片。当永久磁铁靠近射线时,戈尔茨坦无法检测到任何偏转。然而,在1898年,W. Wein通过使用非常强大的磁场,使这些射线偏转,并表明其中一些带正电;通过测量电和磁的偏转,他证明了这些射线中粒子的质量与氢原子的质量相当,因此是阴极射线中粒子质量的一千多倍。这些正射线的组成比阴极射线的组成复杂得多,因为阴极射线中的粒子都是同一种,而正射线中有许多不同种类的粒子。然而,我们可以用下面的方法将这些粒子分类,确定存在什么样的粒子,以及它们运动的速度。假设这些射线中的一束平行于x轴运动,在点O处与平面成直角;如果在它们到达平面之前,它们受到平行于y轴的电力作用,粒子撞击平面的点就会偏转,平行于y,经过一段由方程给出的距离
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Rays of Positive Electricity.
In 1886, Goldstein observed that when the cathode in a vacuum tube was pierced with holes, the electrical discharge did not stop at the cathode; behind the cathode, beams of light could be seen streaming through the holes in the way represented in Figure 1. He ascribed these pencils of light to rays passing through the holes into the gas behind the cathode; and from their association with the channels through the cathode he called these rays Kanalstrahlen. The colour of the light behind the cathode depends on the gas in the tube: with air the light is yellowish, with hydrogen rose colour, with neon the gorgeous neon red, the effects with this gas being exceedingly striking. The rays produce phosphorescence when they strike against the walls of the tube; they also affect a photographic plate. Goldstein could not detect any deflection when a permanent magnet was held near the rays. In 1898, however, W. Wein, by the use of very powerful magnetic fields, deflected these rays and showed that some of them were positively charged; by measuring the electric and magnetic deflections he proved that the masses of the particles in these rays were comparable with the masses of atoms of hydrogen, and thus were more than a thousand times the mass of a particle in the cathode ray. The composition of these positive rays is much more complex than that of the cathode rays, for whereas the particles in the cathode rays are all of the same kind, there are in the positive rays many different kinds of particles. We can, however, by the following method sort these particles out, determine what kind of particles are present, and the velocities with which they are moving. Suppose that a pencil of these rays is moving parallel to the axis of x, striking a plane a right angles to their path at the point O; if before they reach the plane they are acted on by an electric force parallel to the axis of y, the spot where a particle strikes the plane will be deflected parallel to y through a distance y given by the equation
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