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Untitled - Aerobib - Universidad Politécnica de Madrid

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12 CHAPTER 1. THERMOCHEMISTRY<br />

Between these magnitu<strong>de</strong>s the following relations exist<br />

∑<br />

c j =c , (1.27)<br />

j<br />

∑<br />

X j =1 . (1.28)<br />

j<br />

Let ρ be the <strong>de</strong>nsity of the mixture, ρ i the partial <strong>de</strong>nsity of species A i , Y i its<br />

mass fraction and M i its molar mass. The following relations exist<br />

ρ i = ρY i , (1.29)<br />

∑ ∑<br />

ρ j = ρ, Y j = 1 , (1.30)<br />

j<br />

j<br />

c i = ρ M i<br />

Y i , (1.31)<br />

c = ρ ∑ j<br />

Y j<br />

M j<br />

, (1.32)<br />

The mean molar mass M m of the mixture is <strong>de</strong>fined by<br />

X i = ∑<br />

Y i/M i<br />

, (1.33)<br />

Y j /M j<br />

j<br />

Y i = ∑<br />

M iX i<br />

. (1.34)<br />

M j X j<br />

j<br />

M m = ∑ j<br />

M j X j . (1.35)<br />

From Eqs.<br />

following expression<br />

(1.30) and (1.35) one <strong>de</strong>duces for M m as a function of Y i the<br />

1<br />

M m<br />

= ∑ j<br />

Y j<br />

M j<br />

. (1.36)<br />

Equation of state of the mixture<br />

Since the number of moles of the mixture per unit volume is c, one has<br />

p = cRT = RT ∑ j<br />

c j = ∑ j<br />

p j , (1.37)<br />

where<br />

p j = c j RT = R gj T = X j p (1.38)

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