双语化学辞典Chem Lexicon
本科Undergraduate 离子晶体与晶格能 Ionic solids & lattice energy

玻恩–朗德方程Born–Landé equation

\[U_L = -\frac{N_A M z_+ z_- e^2}{4\pi\varepsilon_0 r_0}\left(1 - \frac{1}{n}\right)\]
玻恩–迈耶方程(指数排斥)Born–Mayer equation (exponential repulsion)
\[U_L = -\frac{N_A M |z_+z_-| e^2}{4\pi\varepsilon_0 r_0}\left(1 - \frac{\rho}{r_0}\right)\]

含义Meaning

由离子间库仑吸引与短程排斥计算离子晶体的晶格能(气态离子形成 1 mol 晶体释放的能量)。

Computes the lattice energy of an ionic crystal (energy released when gaseous ions form 1 mol of solid) from Coulomb attraction and short-range repulsion.

符号说明Symbols

符号Symbol含义 Meaning单位 Unit
\(M\)马德隆常数Madelung constant1
\(z_\pm\)离子电荷数(|z|)ionic charges1
\(r_0\)平衡阴阳离子间距equilibrium cation–anion distancem
\(n\)玻恩指数(5–12,取决于电子构型)Born exponent (5–12)1
\(\rho\)排斥范围参数 ≈ 0.345 Årepulsion range parameter ≈ 0.345 Åm

推导Derivation

  1. 一对离子的库仑能 \(z_+z_-e^2/(4\pi\varepsilon_0r)\);对整个晶格求和得到马德隆常数 M(只依赖结构)。

    The Coulomb energy of one pair summed over the lattice gives the Madelung constant M (structure only).

  2. 电子云重叠引起的排斥写作 \(B/r^n\)。每摩尔能量 \(U(r) = -\frac{N_AMz^2e^2}{4\pi\varepsilon_0 r} + \frac{N_AB}{r^n}\)。

    Repulsion from overlapping electron clouds: \(B/r^n\).

  3. 平衡时 \(dU/dr = 0\),解出 \(B = \frac{Mz^2e^2r_0^{\,n-1}}{4\pi\varepsilon_0 n}\)。

    At equilibrium \(dU/dr = 0\), fixing B.

  4. 代回即得 \(U_L = -\frac{N_AMz^2e^2}{4\pi\varepsilon_0r_0}(1 - 1/n)\)。排斥项只修正约 10%。

    Substituting back gives the result; repulsion corrects by only ~10 %.

  5. n 由压缩率测定,或按离子构型取值:He 5、Ne 7、Ar 9、Kr 10、Xe 12(阴阳离子取平均)。

    n from compressibility, or by configuration: He 5, Ne 7, Ar 9, Kr 10, Xe 12 (average for the pair).

适用条件与局限Assumptions & limitations

  • 纯离子模型;对极化强、共价成分大的晶体(AgI、CuCl)计算值明显小于玻恩–哈伯循环实验值。

    Purely ionic; underestimates for polarisable or covalent solids (AgI, CuCl).

  • 忽略范德华色散能与零点能(约 1–2%)。

    Neglects dispersion and zero-point energy (~1–2 %).

例题Worked example

NaCl:M = 1.74756,r₀ = 2.814 Å,n = 8:U_L = −755 kJ/mol(玻恩–哈伯实验值 −787 kJ/mol)。

NaCl: M = 1.74756, r₀ = 2.814 Å, n = 8: U_L = −755 kJ/mol (Born–Haber −787).