含义Meaning
配分函数是按玻尔兹曼因子加权的有效可及态数,包含体系全部热力学信息。分子能量可分解时,配分函数可写成各运动形式配分函数之积。
The partition function counts thermally accessible states weighted by Boltzmann factors and contains all thermodynamic information. When the molecular energy separates, q factorises into contributions from each motion.
符号说明Symbols
| 符号Symbol | 含义 Meaning | 单位 Unit |
|---|---|---|
| \(q\) | 分子配分函数molecular partition function | 1 |
| \(Q\) | 体系(正则)配分函数canonical partition function | 1 |
| \(N\) | 分子数number of molecules | 1 |
推导Derivation
玻尔兹曼分布的归一化因子即 \(q\);T → 0 时 \(q \to g_0\),T → ∞ 时 q 趋于可及态总数。
q normalises the Boltzmann distribution; it tends to \(g_0\) as T → 0 and grows with T.
若 \(\varepsilon = \varepsilon_t + \varepsilon_r + \varepsilon_v + \varepsilon_e\) 且各自独立,指数和可拆成乘积。
If ε = εt + εr + εv + εe independently, the sum factorises.
N 个不可区分分子的体系:交换分子不产生新状态,除以 N! 避免重复计数(吉布斯修正)。
For N indistinguishable molecules divide by N! (Gibbs correction).
适用条件与局限Assumptions & limitations
能量可分离是近似(振–转耦合、非谐性);\(Q = q^N/N!\) 只在经典极限下成立。
Separability is approximate; \(Q = q^N/N!\) holds in the classical limit.