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'''Excess molar quantities''' are properties of mixtures which characterize the nonideal behaviour of real mixtures. They are the difference between the partial molar property of a component in a real mixture and that of the component in an ideal mixture. By definition, excess properties of a mixture are related to those of the pure substances in an ideal mixture by:
 
:<math>z^E=z-\sum_i x_iz^{id}_i.</math>
 
Here <math>*</math> denotes the pure substance, <math>E</math> the excess molar property, and <math>z</math> corresponds to the specific property under consideration. From the definition of partial molar properties,
 
:<math>z=\sum_i x_i \bar{Z_i},</math>
 
substitution yields:
 
:<math>z^E=\sum_i x_i(\bar{Z_i}-z_i^{id}).</math>
For volumes, internal energies and enthalpies the excess quantities are identical to the mixing quantities.
 
==Examples==
The volume of a mixture from the sum of the excess volumes of the components of a mixture is given by the formula:
:<math>
{V} = \sum_i V_i + \sum_i V_i^{E}
</math>
 
Deriving by temperature the thermal expansivities of the components in a mixture can be related to the expansivity of the mixture:
:<math>\frac{\partial V}{\partial T} = \sum_i \frac{\partial V_i}{\partial T} + \sum_i \frac{\partial V_i^{E}}{\partial T}
</math>
Equivalently:
<math>
:\alpha_V V = \sum_i \alpha_{V,i} V_i + \sum_i \frac{\partial V_i^{E}}{\partial T}
</math>
 
Substituting the excess molar volume
:<math>\frac{\partial \bar{V^E}_i}{\partial T} = R \frac{\partial (ln(\gamma_i))}{\partial P} +RT {\partial^2\over\partial T\partial P} ln(\gamma_i)</math>
one can relate activity coefficients to thermal expansivity.
 
==See also==
*[[Apparent molar property]]
*[[Heat of mixing]]
 
==References==
{{cite book | last = Frenkel | first = Daan | authorlink = Daan Frenkel | coauthors = Smit, Berend | title = Understanding Molecular Simulation : from algorithms to applications | publisher = [[Academic Press]] | year = 2001 | location = [[San Diego, California]] | pages = | url = | doi = | id = | isbn = 0-12-267351-4 }}
 
==External links==
* [http://www.springerlink.com/content/c5h0r422j762k416/]
* [http://scitation.aip.org/content/aip/journal/jcp/32/5/10.1063/1.1730921 excess quantities for electrolyte mixtures]
[[Category:Physical quantities]]

Latest revision as of 21:50, 14 May 2013

Excess molar quantities are properties of mixtures which characterize the nonideal behaviour of real mixtures. They are the difference between the partial molar property of a component in a real mixture and that of the component in an ideal mixture. By definition, excess properties of a mixture are related to those of the pure substances in an ideal mixture by:

zE=zixiziid.

Here * denotes the pure substance, E the excess molar property, and z corresponds to the specific property under consideration. From the definition of partial molar properties,

z=ixiZi¯,

substitution yields:

zE=ixi(Zi¯ziid).

For volumes, internal energies and enthalpies the excess quantities are identical to the mixing quantities.

Examples

The volume of a mixture from the sum of the excess volumes of the components of a mixture is given by the formula:

V=iVi+iViE

Deriving by temperature the thermal expansivities of the components in a mixture can be related to the expansivity of the mixture:

VT=iViT+iViET

Equivalently: :αVV=iαV,iVi+iViET

Substituting the excess molar volume

VE¯iT=R(ln(γi))P+RT2TPln(γi)

one can relate activity coefficients to thermal expansivity.

See also

References

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External links