Electron Transitions电子跃迁
The Bohr model for an electron transition in hydrogen between quantized energy levels with different quantum numbers n yields a photon by emission with quantum energy:
![]() This is often expressed in terms of the inverse wavelength or "wave number" as follows: ![]() The reason for the variation of R is that for hydrogen the mass of the orbiting electron is not negligible compared to the proton at the high accuracy at which spectral measurement is done. So the reduced mass of the electron is needed. But for heavier elements the movement of the nucleus can be neglected. R的变化是因为对于氢来说,在进行光谱测量的高精度下,绕行电子的质量与质子相比不可忽略。因此需要使用电子的约化质量。但对于较重的元素,核的运动可以忽略不计。
玻尔模型中,氢原子中量子数不同的能级之间电子跃迁时,通过发射具有量子能量的光子,其能量可表示为:这通常以波数或‘波长倒数’的形式表达如下: |
Index Atomic structure concepts 索引 原子结构概念 | ||
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Hydrogen Energy Levels氢能能级
The basic hydrogen energy level structure is in agreement with the Bohr model. Common pictures are those of a shell structure with each main shell associated with a value of the principal quantum number n. ![]() This Bohr model picture of the orbits has some usefulness for visualization so long as it is realized that the "orbits" and the "orbit radius" just represent the most probable values of a considerable range of values. If the radial probabilities for the states are used to make sure you understand the distributions of the probability, then the Bohr picture can be superimposed on that as a kind of conceptual skeleton. 尽管玻尔模型中的轨道概念在一定程度上有助于可视化,但必须认识到这些“轨道”和“轨道半径”仅代表某一较大范围内值的最可能值。如果使用径向概率分布来确保你理解概率分布,那么玻尔模型可以作为一种概念框架叠加在上面。
氢的基态能量结构与玻尔模型一致。常见的图景是壳层结构,每个主壳层都对应一个主量子数n的值。 |
Index Hydrogen concepts Atomic structure concepts 索引 氢概念 原子结构概念 | ||||
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Hydrogen Energy Level Plot氢能级图
The basic structure of the hydrogen energy levels can be calculated from the Schrodinger equation. The energy levels agree with the earlier Bohr model, and agree with experiment within a small fraction of an electron volt. 氢原子能级的基本结构可以从薛定谔方程中计算出来。这些能级与之前的玻尔模型一致,并且与实验结果在电子伏特的很小范围内一致。
![]() If you look at the hydrogen energy levels at extremely high resolution, you do find evidence of some other small effects on the energy. The 2p level is split into a pair of lines by the spin-orbit effect. The 2s and 2p states are found to differ a small amount in what is called the Lamb shift. And even the 1s ground state is split by the interaction of electron spin and nuclear spin in what is called hyperfine structure. 如果以极高的分辨率观察氢原子的能级,你确实会发现一些其他微小效应对能量的影响。2p电平由于自旋-轨道效应被分裂成两条线。2s和2p态被发现存在微小差异,这种差异被称为朗德移位。甚至1s基态也因电子自旋与核自旋的相互作用而被分裂,这种现象称为超精细结构。
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Index Hydrogen concepts Atomic structure concepts 索引 氢概念 原子结构概念 | ||
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Hydrogen Spectrum氢谱线
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This spectrum was produced by exciting a glass tube of hydrogen gas with about 5000 volts from a transformer. It was viewed through a diffraction grating with 600 lines/mm. The colors cannot be expected to be accurate because of differences in display devices. 这种光谱是通过将氢气玻璃管加上约5000伏电压的变压器激发产生的。它通过一个每毫米有600条线的衍射光栅观察。由于显示器设备的差异,颜色无法保证准确。
Radiation of all the types in the electromagnetic spectrum can come from the atoms of different elements. A rough classification of some of the types of radiation by wavelength is: 电磁谱中所有类型的辐射都可以来自不同元素的原子。按波长对一些辐射类型进行粗略分类如下:
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Index Great experiments of physics Hydrogen concepts Atomic structure concepts 索引 物理学伟大实验 氢概念 原子结构概念 | ||||||
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Measured Hydrogen Spectrum测量的氢谱
The measured lines of the Balmer series of hydrogen in the nominal visible region are:
氢的巴尔末系列在名义可见区域的测量谱线为:氘的红色谱线在656.1065(±0.1787 nm)处有可测量的差异。 |
Index Hydrogen concepts Atomic spectra 索引:氢的概念 原子光谱 | |||||||||||||||||||||||||||||||||||||||||
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Hydrogen Energy Levels氢能能级
![]() Active illustration: click for more detail
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Index Hydrogen concepts Atomic spectra 索引:氢的概念 原子光谱 | ||
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