含义Meaning
玻尔兹曼熵把熵与微观状态数联系起来;吉布斯形式适用于任意概率分布,与信息论的香农熵形式相同。
Boltzmann’s entropy links S to the number of microstates; Gibbs’s form applies to any distribution and matches Shannon’s information entropy.
符号说明Symbols
| 符号Symbol | 含义 Meaning | 单位 Unit |
|---|---|---|
| \(W\) | 与宏观态相容的微观状态数number of microstates | 1 |
| \(p_i\) | 微观态 i 的概率probability of microstate i | 1 |
推导Derivation
熵是广延量,两个独立体系 \(W = W_1W_2\),而 \(S = S_1 + S_2\),只有对数函数满足 \(f(W_1W_2) = f(W_1) + f(W_2)\)。
S is extensive while W multiplies; only the logarithm turns products into sums.
等概率 \(p_i = 1/W\) 时吉布斯形式化为 \(k\ln W\)。
With equal probabilities 1/W the Gibbs form reduces to k ln W.
代入玻尔兹曼分布 \(p_i = e^{-\beta E_i}/Q\):\(S = U/T + k_\mathrm{B}\ln Q\)。
Inserting Boltzmann probabilities gives \(S = U/T + k\ln Q\).
残余熵:CO 晶体中分子取向 CO/OC 随机,\(S = R\ln 2 = 5.76\ \mathrm{J/(mol\,K)}\)(实测约 4.6)。
Residual entropy: random CO/OC orientations give R ln 2 = 5.76 J mol⁻¹ K⁻¹ (observed ≈ 4.6).
适用条件与局限Assumptions & limitations
W 的计数需正确处理全同粒子(量子统计)。
Counting must handle identical particles correctly.