Mr.Hope

第二章

Mr.Hope ... 2020-12-28 物理
  • 热统
 大约 2 分钟

# 四个热力学函数

H=U+pVF=U−TSG=U−TS+pV\begin{aligned} H =& U + pV\\ F =& U - TS\\ G =& U - TS + pV \end{aligned}

微分形式:

U=TdS−pdVU = TdS - pdV

F=−SdT−pdVF = -SdT - pdV

H=TdS+VdpH = TdS + Vdp

G=−SdT+VdpG = -SdT + Vdp

H=G−T∂G∂TH=G-T\frac{\partial G}{\partial T}

U=F−T∂F∂T=G−T∂G∂T−p∂G∂pU=F-T\frac{\partial F}{\partial T} =G-T\frac{\partial G}{\partial T}-p\frac{\partial G}{\partial p}

# 麦克斯韦关系

(∂T∂V)S=−(∂p∂S)V(\frac{\partial T}{\partial V})_S = -(\frac{\partial p}{\partial S})_V

(∂T∂p)S=(∂V∂S)p(\frac{\partial T}{\partial p})_S = (\frac{\partial V}{\partial S})_p

(∂S∂V)T=(∂p∂T)V(\frac{\partial S}{\partial V})_T = (\frac{\partial p}{\partial T})_V

(∂S∂p)T=−(∂V∂T)p(\frac{\partial S}{\partial p})_T = -(\frac{\partial V}{\partial T})_p

一些扩展:

Cv=(∂U∂T)V=T(∂S∂T)VC_v = (\frac{\partial U}{\partial T})_V = T (\frac{\partial S}{\partial T})_V

Cp=(∂U∂T)p+p(∂V∂T)p=(∂H∂T)p=T(∂S∂T)pC_p = (\frac{\partial U}{\partial T})_p + p (\frac{\partial V}{\partial T})_p = (\frac{\partial H}{\partial T})_p = T (\frac{\partial S}{\partial T})_p

(∂U∂V)T=T(∂p∂T)V−p=Tpβ−p(\frac{\partial U}{\partial V})_T = T(\frac{\partial p}{\partial T})_V - p = \frac{T}{p}\beta - p

(∂H∂p)T=V−T(∂V∂T)p=V−TVα(\frac{\partial H}{\partial p})_T = V - T(\frac{\partial V}{\partial T})_p = V - \frac{T}{V}\alpha

# 节流过程

气体在节流过程中焓不变。

μ=(∂T∂p)H=VCp(Tα−1)=1Cp[T(∂V∂T)p−V]\mu=(\cfrac{\partial T}{\partial p})_H = \cfrac{V}{C_p}(T\alpha - 1)=\cfrac{1}{C_p}[T(\cfrac{\partial V}{\partial T})_p -V] 称为焦汤系数。

可以利用节流过程中 μ>0\mu > 0 一侧制冷区，利用节流过程使得液体降温而液化。

# 内能与焓的积分形式

U=∫{CvdT+[T(∂p∂T)V−p]dV}+U0U = \int\{C_vdT+[T(\frac{\partial p}{\partial T})_V -p]dV\}+U_0

S=∫[CvTdT+(∂p∂TdV)]+S0S = \int[\frac{C_v}{T}dT+(\frac{\partial p}{\partial T}dV)]+S_0

# 热辐射

辐射压强 p=13up=\cfrac{1}{3}u，而能态密度 u=aT4u=aT^4。

S=43aT3VS=\cfrac{4}{3}aT^3V (可逆绝热下有 T3VT^3V 常数)

辐射通量密度 Ju=14CUJ_u=\cfrac{1}{4}CU

# 磁介质

m=MVm=MV 是介质的总磁矩

所做的功为 dW=μ0HdmdW =\mu_0Hdm

磁介质的内能满足 dU=TdS+μ0hdmdU=TdS+\mu_0hdm

磁介质的吉布斯函数满足 dG=−SdT−μ0mdHdG=-SdT-\mu_0mdH

磁介质的热容 CH=T(∂S∂T)HC_H=T(\cfrac{\partial S}{\partial T})_H 则 (∂T∂H)S=−μ0TCH(∂m∂T)M(\cfrac{\partial T}{\partial H})_S=-\cfrac{\mu_0T}{C_H}(\cfrac{\partial m}{\partial T})_M

居里定律: m=CVTHm=\cfrac{C_V}{T}H 可以得出: (∂T∂H)S=CVCHTμ0H(\cfrac{\partial T}{\partial H})_S=\cfrac{C_V}{C_HT}\mu_0H 和 TdS=CVdT+TακTdVTdS =C_VdT+T\cfrac{\alpha}{\kappa_T}dV

# 重要习题

  1. 证明 κsκT=CvCp\cfrac{\kappa_s}{\kappa_T} = \cfrac{C_v}{C_p}

  2. 证明 Cp−CV=−T(∂p∂T)V2(∂p∂V)TC_p - C_V = -T\cfrac{(\cfrac{\partial p}{\partial T})_V^2}{(\cfrac{\partial p}{\partial V})_T}

第三章