Compressibility: Difference between revisions

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The  '''isothermal compressibility''',  <math>\kappa_T</math> is given by
The  '''isothermal compressibility''',  <math>\kappa_T</math> is given by


:<math>\kappa_T =-\frac{1}{V} \left.\frac{\partial V}{\partial P}\right\vert_{T} =  \frac{1}{\rho} \left.\frac{\partial \rho}{\partial P}\right\vert_{T}</math>
:<math>\kappa_T =-\frac{1}{V} \left.\frac{\partial V}{\partial p}\right\vert_{T} =  \frac{1}{\rho} \left.\frac{\partial \rho}{\partial p}\right\vert_{T}</math>


(Note: in Hansen and McDonald the isothermal compressibility is written as <math>\chi_T</math>).
(Note: in Hansen and McDonald the isothermal compressibility is written as <math>\chi_T</math>).

Revision as of 14:11, 21 June 2007

The compressibility, Z, is given by

Z=pVNkBT

The bulk modulus B gives the change in volume of a solid substance as the pressure on it is changed,

B=−V∂P∂V

The compressibility K or κ, is given by

κ=1B

The isothermal compressibility, κT is given by

κT=−1V∂V∂p|T=1ρ∂ρ∂p|T

(Note: in Hansen and McDonald the isothermal compressibility is written as χT). where ρ is the particle number density given by

ρ=NV

where N is the total number of particles in the system, i.e.

N=∫Vρ(r,t)dr

See also

The compressibility equation in statistical mechanics.

Compressibility of an Ideal Gas

From the ideal gas law we see that

Z=pVNkBT=1