Thiele hard sphere equation of state: Difference between revisions
		
		
		
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|  (Added the Thiele equation) |  (Mentioned the Carnahan-Starling equation) | ||
| Line 12: | Line 12: | ||
| :<math>\eta</math> is the [[packing fraction]] of the fluid. | :<math>\eta</math> is the [[packing fraction]] of the fluid. | ||
| In terms of accuracy, the Thiele equation is superseded by the [[Carnahan-Starling equation of state]] | |||
| [[category: Equations of state]] | [[category: Equations of state]] | ||
| [[category: hard sphere]] | [[category: hard sphere]] | ||
Revision as of 20:25, 10 February 2021
The Thiele hard sphere equation of state is an equation of state for a hard sphere fluid developed by Thiele in 1963. The equation provides a better approximation of the repulsive forces between molecules than the Van der Waals repulsive term. The equation is given below:
,
where:
- is the compressibility factor of the hard sphere fluid;
- is the pressure of the fluid;
- is the molar volume of the fluid;
- is the absolute temperature of the fluid;
- is the gas constant; and
- is the packing fraction of the fluid.
In terms of accuracy, the Thiele equation is superseded by the Carnahan-Starling equation of state
