Basic Definations

System & Surroundings

system – part

surroundings – everything outside the system

Tips

If the universe is regarded as the universal set(全集), then the surroundings is the complement(补集) of the system.

Types of systems:

  • Open system

Exchanges energy and matter with surroundings

  • Closed system

Exchanges energy but no matter

  • Isolated system

Exchanges no energy or matter

State Functions & Path Functions

State: $U,H,S,G$

Path: $q,w$

Extensive Properties & Intensive Properties

Extensive properties depend on the amount of matter, $V$

Intensive properties do not depend on the amount of matter, $T,V_m$

Thermodynamic Processes

  • Isothermal
  • Isobaric
  • Isochoric
  • Adiabatic
  • Reversible
  • Irreversible

Internal Energy, Enthalpy & Heat Capacity

Basic Defination

  • Energy
  • Internal Energy $U$
  • Work $w$

First Law of Thermodynamics

$$\Delta U=q+w$$

为什么 $q$和 $w$是path function,而 $U$却为state function呢?

https://www.quora.com/How-entropy-is-a-state-function

Enthalpy

$$H=U+pV$$

$U,p,V$均为state function,$H$也为state function.

无法直接测量$H$,只能通过热量变化$q_p$间接测$\Delta H$;$\Delta H<0$为exothermic,$\Delta H>0$为吸热反应.

Heat Capacity $C$

热容(heat capacity, $C$)描述系统升高 1K 所需的热量,是能量储存能力的度量:

$$C = \frac{\delta q}{dT}$$

按 “是否考虑物质的量” 和 “过程条件” 可分为:

  1. 按物质的量分类
  2. 按过程条件分类

按物质的量分类

  • 比热容(specific heat capacity, $C_s$)

单位质量的热容,$C_s= C/m$(m 为质量)

  • 摩尔热容(molar heat capacity,C_m):单位物质的量的热容,$C_m = C/n$(n 为物质的量);

注意:部分文献省略 “m”,需通过单位判断(Cₘ单位为 J・K⁻¹・mol⁻¹,C 为 J・K⁻¹)

按过程条件分类

  • 定容热容(constant volume heat capacity, $C_v$)

等容过程(dV=0)中,$\delta q_v = dU$,因此:$C_V = \left( \frac{\partial U}{\partial T} \right)_V$(偏导数表示 “体积固定时,$U$ 随 $T$ 的变化率”),且 $dU = C_v dT$

  • 定压热容(constant pressure heat capacity, $C_p$)

等压过程($dp=0$)中,$\delta q_p = dH$,因此:$C_p = \left( \frac{\partial H}{\partial T} \right)_p$且 $dH = C_p dT$

$C_p$与$C_v$的关系

固体 / 液体:$C_p \approx C_v$(体积变化小,膨胀功可忽略,ΔU≈ΔH)

理想气体:$C_p = C_v + nR$($R$ 为气体常数)

示例:单原子理想气体(如 He)的 Cᵥ,m = 3R/2,Cₚ,m = 5R/2(由能量均分原理推导)


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