Question #60826

I just need help to solve a problem:

Show that (∂E/∂V)β, N + β(∂p/∂β)N, V = - p

PS: There is a bar over E and over p (this in both sides) - meaning that is an average.

Expert's answer

Answer on Question #60826 - Physics - Molecular Physics | Thermodynamics

Show that (EV)β,N+β(pβ)N,V=p\left(\frac{\partial E}{\partial V}\right)_{\beta ,N} + \beta \left(\frac{\partial p}{\partial \beta}\right)_{N,V} = -p

Solution:


dβ=βTdTβ(pβ)=βTβ(pT)=T(pT)=T(SV)d \beta = - \frac {\beta}{T} d T \Rightarrow \beta \left(\frac {\partial p}{\partial \beta}\right) = - \frac {\beta T}{\beta} \left(\frac {\partial p}{\partial T}\right) = - T \left(\frac {\partial p}{\partial T}\right) = - T \left(\frac {\partial S}{\partial V}\right)dE=TdSpdVEV=T(SV)pEVT(SV)=EV+β(pβ)=pd E = T d S - p d V \Rightarrow \frac {\partial E}{\partial V} = T \left(\frac {\partial S}{\partial V}\right) - p \Rightarrow \frac {\partial E}{\partial V} - T \left(\frac {\partial S}{\partial V}\right) = \frac {\partial E}{\partial V} + \beta \left(\frac {\partial p}{\partial \beta}\right) = - pEV=0 (Joule’s law)\frac {\partial E}{\partial V} = 0 \text{ (Joule's law)}β(pβ)=T(SV)=T(pT)=TRdTVdT=RTV=p\beta \left(\frac {\partial p}{\partial \beta}\right) = - T \left(\frac {\partial S}{\partial V}\right) = - T \left(\frac {\partial p}{\partial T}\right) = - T \frac {R d T}{V d T} = - R \frac {T}{V} = - p0p=p(EV)+β(pβ)=p0 - p = - p \Rightarrow \left(\frac {\partial E}{\partial V}\right) + \beta \left(\frac {\partial p}{\partial \beta}\right) = - p


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