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Low Densities The Virial Equation

We know that as the density p approaches zero at a constant temperature T, the product (PV) remains finite and becomes equal to NkT at the limit p = 0, i.e. z = 1, at p = 0. [Pg.624]

A Maclaurin s series expansion in density around p = 0 yields  [Pg.624]

In Chapter 8 we used B for the second virial coefficient, C for the third, and so on. Here we use, for generality, 82,8, etc. 8 is the unity that appears before the summation. [Pg.624]

We also stated that the virial coefficients of pure compounds are functions of temperature only. This is apparent here, because they are defined at the limit p = 0, at a specified temperature. [Pg.625]

The virial equation was first proposed by Kammerlingh Onnes in 1901 on a purely empirical basis he also suggested the name void. [Pg.625]


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