双语化学辞典Chem Lexicon
概念 · 物理化学 · 热力学 Physical chemistry · Thermodynamics

熵Entropy

高中High school
拼音Pinyin shāng 

定义Definition

熵是描述体系中能量与粒子分散程度的状态函数,符号 S,单位 J K⁻¹ mol⁻¹(摩尔熵)。从统计角度,S = k ln W,W 为体系可能的微观状态数;微观状态越多,熵越大。

Entropy, S, is a state function measuring how dispersed the energy and particles of a system are, in J K⁻¹ mol⁻¹ for molar entropy. Statistically S = k ln W, where W is the number of possible microstates; the more microstates, the higher the entropy.

比较熵的大小Comparing entropies

同一物质:气态 > 液态 > 固态,如 H₂O(g) 188.8、H₂O(l) 69.9 J K⁻¹ mol⁻¹。温度升高熵增大。粒子越多、结构越复杂,熵越大。反应生成更多气体分子时熵增加,如 CaCO₃(s) → CaO(s) + CO₂(g) 的 ΔS 为正。完美晶体在 0 K 时熵为零(热力学第三定律)。

For one substance, gas > liquid > solid: H₂O(g) 188.8 and H₂O(l) 69.9 J K⁻¹ mol⁻¹. Entropy rises with temperature, and with more particles and more complex structures. Reactions that produce more gas molecules increase entropy, so ΔS for CaCO₃(s) → CaO(s) + CO₂(g) is positive. A perfect crystal at 0 K has zero entropy (the third law).

与自发性的关系Link to feasibility

热力学第二定律:孤立体系的总熵永不减少。判断恒温恒压下反应能否自发,要同时考虑焓变和熵变:ΔG = ΔH − TΔS,ΔG < 0 时反应可自发进行。例如 ΔH > 0、ΔS > 0 的反应在高温下才能自发。

The second law states that the total entropy of an isolated system never decreases. At constant temperature and pressure, feasibility depends on both enthalpy and entropy: ΔG = ΔH − TΔS, and a reaction is feasible when ΔG < 0. A reaction with ΔH > 0 and ΔS > 0, for example, becomes feasible only at high temperature.

计算Calculation

ΔS°(反应) = Σ S°(生成物) − Σ S°(反应物),注意乘以化学计量数,单位 J K⁻¹ mol⁻¹;代入 ΔG = ΔH − TΔS 时要换算成 kJ。

ΔS°(reaction) = Σ S°(products) − Σ S°(reactants), multiplied by the coefficients, in J K⁻¹ mol⁻¹; convert to kJ before using ΔG = ΔH − TΔS.

年表Timeline

  • 1865

    克劳修斯提出“熵”的概念并命名

    Clausius introduces and names entropy

  • 1877

    玻尔兹曼给出熵的统计解释 S = k ln W

    Boltzmann gives the statistical interpretation S = k ln W

  • 1906

    能斯特提出热定理,后发展为热力学第三定律

    Nernst states his heat theorem, later the third law of thermodynamics

相关公式Formulas

熵与克劳修斯不等式(第二定律) Entropy and the Clausius inequality (second law)→
\[dS = \frac{\delta q_\text{rev}}{T},\qquad dS \ge \frac{\delta q}{T},\qquad \Delta S_\text{孤立} \ge 0\]\[dS = \frac{\delta q_\text{rev}}{T},\qquad dS \ge \frac{\delta q}{T},\qquad \Delta S_\text{isolated} \ge 0\]
变温过程的熵变 Entropy change on heating→
\[\Delta S = \int_{T_1}^{T_2}\frac{C_p}{T}dT = C_p\ln\frac{T_2}{T_1}\ (\text{恒压,} C_p\text{ 恒定}),\qquad \Delta S = nC_{V,m}\ln\frac{T_2}{T_1} + nR\ln\frac{V_2}{V_1}\]\[\Delta S = \int_{T_1}^{T_2}\frac{C_p}{T}dT = C_p\ln\frac{T_2}{T_1}\ (\text{const. p ,} C_p\text{const.}),\qquad \Delta S = nC_{V,m}\ln\frac{T_2}{T_1} + nR\ln\frac{V_2}{V_1}\]
例题Worked example

1 mol 水从 0 °C 加热到 100 °C:ΔS = 75.3×ln(373/273) = 23.5 J/K。

Heating 1 mol of water 0 → 100 °C: ΔS = 23.5 J/K.

相变熵 Entropy of phase transition→
\[\Delta_\text{trs}S = \frac{\Delta_\text{trs}H}{T_\text{trs}}\]
例题Worked example

水汽化:ΔS = 40.7×10³/373 = 109 J/(mol·K);冰融化:6.01×10³/273 = 22.0 J/(mol·K)。

Water: ΔvapS = 109, ΔfusS = 22.0 J mol⁻¹ K⁻¹.

统计熵 Statistical entropy→
\[S = k_\mathrm{B}\ln W,\qquad S = -k_\mathrm{B}\sum_i p_i\ln p_i\]