Coomber's relationship

Coomber's relationship can be used to describe how the internal pressure and dielectric constant of a non-polar liquid are related.

As p i = ( E V ) T {\displaystyle p_{i}=\left({\frac {\partial E}{\partial V}}\right)_{T}\,} , which defines the internal pressure of a liquid, it can be found that:

p i = n I b ( T ) N 2 α 2 V n + 1 {\displaystyle p_{i}=n\cdot I\cdot b(T){\frac {N^{2}\alpha ^{2}}{V^{n+1}}}}
where

  • N {\displaystyle N} is equal to the number of molecules
  • I {\displaystyle I} is the ionization potential of the liquid
  • b ( T ) {\displaystyle b(T)} is a temperature dependent relation based on numerical constants of the pair summation from inter-particle geometry
  • α {\displaystyle \alpha } is the polarizability
  • V {\displaystyle V} is the volume of the liquid

where for most non-polar liquids n = 1 {\displaystyle n=1}

References

  • Meeten, G.H., "Theoretical Basis for Coomber's Relationship", Nature Vol. 223, August 23, 1969


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