Algebraic cycle: Difference between revisions

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In [[statistical mechanics]] and [[thermodynamics]] the '''compressibility equation''' refers to an equation which relates the isothermal [[compressibility]] (and indirectly the pressure) to the structure of the liquid. It reads:
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<math>kT\left(\frac{\partial \rho}{\partial p}\right)=1+\rho \int d r [g(r)-1] </math>    (1)
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where <math>\rho</math> is the number density, g(r) is the [[radial distribution function]] and <math>kT\left(\frac{\partial \rho}{\partial p}\right)</math> is the isothermal [[compressibility]].
 
Using the Fourier representation of the [[Ornstein-Zernike equation]] the compressibility equation (1) can be rewritten in the form:
 
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<math>\frac{1}{kT}\left(\frac{\partial p}{\partial \rho}\right) = \frac{1}{1+\rho \int h(r) d \rm{r}}=\frac{1}{1+\rho \hat{H}(0)}=1-\rho\hat{C}(0)=1-\rho \int c(r) d \rm{r} </math>    (2)
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where h(r) and c(r) are the indirect and direct correlation functions respectively. The compressibility equation is one of the many [[integral equations]] in [[statistical mechanics]].
 
==References==
 
#D.A. McQuarrie, Statistical Mechanics (Harper Collins Publishers) 1976
 
[[Category:Statistical mechanics]]
[[Category:Thermodynamic equations]]

Latest revision as of 13:30, 12 May 2014

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