双语化学辞典Chem Lexicon
概念 · 原子结构 · 原子光谱 Atomic structure · Atomic spectra

氢原子光谱Hydrogen spectral series

拼音Pinyin qīng yuán zǐ guāng pǔ 别名Also 巴耳末系;莱曼系;帕邢系;Balmer series;Lyman series; Paschen series

定义Definition

氢原子光谱是氢原子中电子在不同能级之间跃迁时发射或吸收的一系列分立谱线。按终态能级分为莱曼系(n = 1,紫外)、巴耳末系(n = 2,可见)、帕邢系(n = 3,红外)等,其波长可由里德伯公式精确计算。

The hydrogen spectrum is the set of discrete lines emitted or absorbed when hydrogen's electron jumps between energy levels. By the lower level the series are Lyman (n = 1, ultraviolet), Balmer (n = 2, visible), Paschen (n = 3, infrared) and others, and their wavelengths follow the Rydberg formula precisely.

规律与解释Regularities and explanation

巴耳末系的四条可见谱线为 656.3 nm(红,Hα)、486.1 nm(蓝绿,Hβ)、434.0 nm(蓝紫,Hγ)和 410.2 nm(紫,Hδ),向短波方向逐渐密集,收敛于系限 364.6 nm。玻尔模型把谱线解释为电子从高能级 n₂ 跃迁到低能级 n₁ 时放出光子,能量 hν = Eₙ₂ − Eₙ₁ = 13.6 eV × (1/n₁² − 1/n₂²)。谱线的分立性直接证明了原子能量的量子化。

The four visible Balmer lines are at 656.3 nm (red, Hα), 486.1 nm (blue-green, Hβ), 434.0 nm (violet, Hγ) and 410.2 nm (violet, Hδ); they crowd together toward shorter wavelength and converge on the series limit at 364.6 nm. The Bohr model explains each line as a photon emitted when the electron falls from level n₂ to n₁, with hν = Eₙ₂ − Eₙ₁ = 13.6 eV × (1/n₁² − 1/n₂²). The discreteness of the lines directly proves that atomic energies are quantised.

发现史History

1885 年瑞士中学教师巴耳末找到可见谱线波长的经验公式 λ = B·n²/(n² − 4)。1888 年里德伯推广为普遍公式。1906 年莱曼发现紫外系,1908 年帕邢发现红外系,之后又发现布拉开系(1922)、普丰德系(1924)和汉弗莱斯系(1953)。1913 年玻尔的原子模型首次从理论上导出这些规律。精细结构和兰姆位移(1947)的发现推动了相对论量子力学和量子电动力学的发展。

In 1885 the Swiss schoolteacher Johann Balmer found an empirical formula for the visible lines, λ = B·n²/(n² − 4), which Rydberg generalised in 1888. Lyman found the ultraviolet series in 1906 and Paschen the infrared series in 1908, followed by the Brackett (1922), Pfund (1924) and Humphreys (1953) series. Bohr's 1913 atomic model first derived these regularities theoretically. Fine structure and the Lamb shift (1947) drove the development of relativistic quantum mechanics and quantum electrodynamics.

应用Applications

天文学中利用 Hα 线观测星云和太阳色球;通过谱线红移测定星系退行速度。氢的 21 cm 超精细跃迁谱线用于绘制银河系的结构。氢光谱的精密测量是检验量子电动力学和测定里德伯常数、质子半径的重要手段。

Astronomers use the Hα line to observe nebulae and the solar chromosphere, and the redshift of hydrogen lines to measure the recession of galaxies. The 21 cm hyperfine line of hydrogen maps the structure of the Milky Way. Precision hydrogen spectroscopy tests quantum electrodynamics and determines the Rydberg constant and the proton radius.

反应Reactions

1/λ = R_H·(1/n12 − 1/n22),R_H ≈ 1.0968 × 107 m−1

n₂ > n₁,均为正整数。

n₂ > n₁, both positive integers.

Hα:n = 3 ⟶ 2,1/λ = R_H(1/4 − 1/9) ⟶ λ ≈ 656 nm

红色巴耳末线

The red Balmer line

莱曼 α:n = 2 ⟶ 1,λ ≈ 121.6 nmα: n = 2 ⟶ 1, λ ≈ 121.6 nm

紫外区最强线

The strongest ultraviolet line

年表Timeline

  • 1885

    巴耳末公式

    Balmer's formula

  • 1888

    里德伯公式

    Rydberg's formula

  • 1906

    莱曼系发现

    The Lyman series is found

  • 1913

    玻尔模型解释氢光谱

    The Bohr model explains the hydrogen spectrum

  • 1947

    兰姆位移发现

    The Lamb shift is discovered

相关公式Formulas

里德伯公式(氢原子光谱) Rydberg formula (hydrogen spectrum)→
\[\tilde\nu = \frac1\lambda = R_\mathrm HZ^2\left(\frac{1}{n_1^2} - \frac{1}{n_2^2}\right),\qquad R_\mathrm H = 1.09678\times10^{7}\ \mathrm m^{-1}\]
例题Worked example

巴耳末 Hα:1/λ = R_H(1/4 − 1/9) → λ = 656.3 nm(红);Hβ 486.1 nm;Hγ 434.0 nm;Hδ 410.2 nm。

Balmer lines: Hα 656.3, Hβ 486.1, Hγ 434.0, Hδ 410.2 nm.