Acentric factor: Difference between revisions
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The ''''' |
The '''''acentric''''' factor <math>\omega</math> is a conceptual number introduced by Pitzer in 1955, proven to be very useful in the description of matter. It has become a standard for the phase characterization of single & pure components. The other state description parameters are [[molecular weight]], [[critical temperature]], [[critical pressure]], and [[critical volume]].'''The a-centric factor''' is said to be a measure of the non-sphericity (centricity) of molecules. |
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It is defined as: |
It is defined as: |
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Values of <math>\omega</math> can be determined for any fluid from <math>\{T_r, p_r\}</math>, and a vapor measurement from <math>T_r = 0.7K</math>, and for many liquid state matteris tabulated into many thermodynamical tables. |
Values of <math>\omega</math> can be determined for any fluid from <math>\{T_r, p_r\}</math>, and a vapor measurement from <math>T_r = 0.7K</math>, and for many liquid state matteris tabulated into many thermodynamical tables. |
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The definition of <math>\omega</math> gives zero-value for [[ |
The definition of <math>\omega</math> gives zero-value for the [[noble gas]]es [[argon]], [[krypton]], and [[xenon]]. |
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Experimental data yields compressibility factors for all fluids that are correlated by the same curves when <math>Z</math> ([[compressibility factor]]) is represented as a function of <math>T_r</math> and <math>p_r</math>. This is the basis premises of [[three-parameter theorem of corresponding states]]: |
Experimental data yields compressibility factors for all fluids that are correlated by the same curves when <math>Z</math> ([[compressibility factor]]) is represented as a function of <math>T_r</math> and <math>p_r</math>. This is the basis premises of [[three-parameter theorem of corresponding states]]: |
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Revision as of 04:32, 4 March 2011
The acentric factor is a conceptual number introduced by Pitzer in 1955, proven to be very useful in the description of matter. It has become a standard for the phase characterization of single & pure components. The other state description parameters are molecular weight, critical temperature, critical pressure, and critical volume.The a-centric factor is said to be a measure of the non-sphericity (centricity) of molecules.
It is defined as:
- .
where is the reduced temperature, is the reduced pressure saturation of vapors.
For many monoatomic, fluids
- at T_r = 0.7,
is close to 0.1, therefore . In many cases, lies abovew the boiling temperature of gases at atmosphere pressure.
Values of can be determined for any fluid from , and a vapor measurement from , and for many liquid state matteris tabulated into many thermodynamical tables.
The definition of gives zero-value for the noble gases argon, krypton, and xenon. Experimental data yields compressibility factors for all fluids that are correlated by the same curves when (compressibility factor) is represented as a function of and . This is the basis premises of three-parameter theorem of corresponding states:
All fluids at any -value, in conditions, have about the same -value, and same degree of convergence.[citation needed]