Compressibility: Difference between revisions
		
		
		
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| Carl McBride (talk | contribs) No edit summary | Carl McBride (talk | contribs)  mNo edit summary | ||
| Line 18: | Line 18: | ||
| where <math>N</math> is the total number of particles in the system, i.e. | where <math>N</math> is the total number of particles in the system, i.e. | ||
| :<math>N = \int_V \rho(r,t)~{\rm d}r</math> | :<math>N = \int_V \rho({\mathbf r},t)~{\rm d}{\mathbf r}</math> | ||
| ==See also== | ==See also== | ||
| The [[compressibility equation]] in [[statistical mechanics]]. | The [[compressibility equation]] in [[statistical mechanics]]. | ||
| [[category:classical thermodynamics]] | [[category:classical thermodynamics]] | ||
Revision as of 14:59, 10 July 2007
The bulk modulus B gives the change in volume of a solid substance as the pressure on it is changed,
The compressibility K or , is given by
The isothermal compressibility, is given by
(Note: in Hansen and McDonald the isothermal compressibility is written as ). where is the particle number density given by
where is the total number of particles in the system, i.e.