Characteristic X-Rays特征X射线
X-ray production typically involves bombarding a metal target in an x-ray tube with high speed electrons which have been accelerated by tens to hundreds of kilovolts of potential. The bombarding electrons can eject electrons from the inner shells of the atoms of the metal target. Those vacancies will be quickly filled by electrons dropping down from higher levels, emitting x-rays with sharply defined frequencies associated with the difference between the atomic energy levels of the target atoms. X射线的产生通常涉及将高能电子轰击金属靶,这些电子在X射线管中被加速至数十到数百千伏的电压。轰击电子可以从金属靶原子的内层壳层中击出电子。这些空位会很快被来自更高能级的电子填补,从而发射出频率明确的X射线,这些X射线与靶原子能级之间的能量差有关。
The frequencies of the characteristic x-rays can be predicted from the Bohr model. Moseley measured the frequencies of the characteristic x-rays from a large fraction of the elements of the periodic table and produced a plot of them which is now called a "Moseley plot". 特征X射线的频率可以从玻尔模型中预测。莫赛尔测量了大量元素的特征X射线频率,并绘制了这些数据,现在称为“莫赛尔图”。
Characteristic x-rays are used for the investigation of crystal structure by x-ray diffraction. Crystal lattice dimensions may be determined with the use of Bragg's law in a Bragg spectrometer. 特征X射线用于通过X射线衍射来研究晶体结构。晶体晶格尺寸可以利用布拉格定律在布拉格谱仪中测定。
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Bremsstrahlung X-RaysBremsstrahlung X射线
![]() "Bremsstrahlung" means "braking radiation" and is retained from the original German to describe the radiation which is emitted when electrons are decelerated or "braked" when they are fired at a metal target. Accelerated charges give off electromagnetic radiation, and when the energy of the bombarding electrons is high enough, that radiation is in the x-ray region of the electromagnetic spectrum. It is characterized by a continuous distribution of radiation which becomes more intense and shifts toward higher frequencies when the energy of the bombarding electrons is increased. The curves above are from the 1918 data of Ulrey, who bombarded tungsten targets with electrons of four different energies. 'Bremsstrahlung' 意为 '制动辐射',保留原德语术语以描述当电子被减速或'制动'时,撞击金属靶时发出的辐射。加速的电荷会发出电磁辐射,当撞击电子的能量足够高时,这种辐射会进入电磁谱的X射线区域。其特征是辐射具有连续分布,当撞击电子的能量增加时,辐射强度增大且向更高频率转移。上方的曲线来自1918年Ulrey的数据,他用四种不同能量的电子轰击钨靶。
The bombarding electrons can also eject electrons from the inner shells of the atoms of the metal target, and the quick filling of those vacancies by electrons dropping down from higher levels gives rise to sharply defined characteristic x-rays. 轰击电子也可以从金属靶原子的内层壳层中逐出电子,这些 vacancies 由来自更高能级的电子迅速填补,从而产生特征 X 射线。
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