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Modern Engineering Thermodynamics

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12.3 Mixtures of Ideal Gases 413<br />

Then, Eq. (12.6) can be used to find<br />

^v i =<br />

<br />

∂V <br />

m<br />

= R ∂m i p m,T m,m j<br />

M i<br />

<br />

Tm<br />

p m<br />

<br />

= R iT m<br />

p m<br />

= v i (12.16)<br />

where v i is the specific volume of gas i at the pressure and temperature of the mixture. Similarly, using the<br />

appropriate equations for the partial specific internal energy ^u i , enthalpy ^h i ,andentropy^s i , we can show that,<br />

for a mixture of ideal gases with constant specific heats, the partial specific properties of gas i in the mixture are<br />

the same as the corresponding specific properties; that is,<br />

and<br />

where T 0 and p 0 are arbitrary reference state values.<br />

^u i = c vi ðT m − T 0 Þ<br />

^h i = c pi ðT m − T 0 Þ<br />

^s i = s i = c pi lnðT m /T 0 Þ − R i lnðp m /p 0 Þ<br />

These relations were also discovered experimentally in the 19th century and are now known as the Gibbs-Dalton<br />

and Amagat laws. In 1801, John Dalton (1766–1844) carried out a series of experiments that led him to conclude<br />

that the total pressure p m of a mixture of ideal gases was equal to the sum of the partial pressures of the<br />

individual component gases in the mixture, where the partial pressure p i of gas i in a mixture of ideal gases is<br />

the pressure gas i would exert if it alone occupied the volume of the mixture at the temperature of the mixture.<br />

This is known as Dalton’s law of partial pressures, and it can be written as<br />

where<br />

p m = ∑ N<br />

i=1<br />

p i = p 1 + p 2 + p 3 + + p N (12.17)<br />

p i = m iR i T m<br />

V m<br />

(12.18)<br />

Later, Emile Amagat (1841–1915) discovered experimentally that the total volume V m of a mixture of ideal<br />

gases was equal to the sum of the partial volumes V i of the individual component gases in the mixture, where<br />

the partial volume V i of gas i in a mixture of ideal gases is the volume gas i would occupy if it alone was at<br />

thepressureandtemperatureofthemixture.ThisisknownasAmagat’s law of partial volumes, anditcanbe<br />

written as<br />

where<br />

V m = ∑ N<br />

i=1<br />

V i = V 1 + V 2 + V 3 + + V N (12.19)<br />

V i = m iR i T m<br />

p m<br />

<br />

or v i = R <br />

iT m<br />

p m<br />

(12.20)<br />

WHAT IS DALTON’S LAW OF PARTIAL PRESSURES?<br />

Dalton’s law of partial pressures states that the partial pressure p i of ideal gas i in a mixture of ideal gases is equal to the<br />

pressure gas i would exert if it alone occupied the volume of the mixture at the temperature of the mixture.<br />

WHAT IS AMAGAT’S LAW OF PARTIAL VOLUMES ?<br />

Amagat’s law of partial volumes states that the partial volume V i of ideal gas i in a mixture of ideal gases is equal to the<br />

volume gas i would occupy if it alone was at pressure and temperature of the mixture.

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