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Untitled - Aerobib - Universidad Politécnica de Madrid

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40 CHAPTER 2. TRANSPORT PHENOMENA IN GAS MIXTURES<br />

Formula (2.7) shows that there are three causes for diffusion corresponding to the three<br />

terms in the right hand si<strong>de</strong> of the equation. Namely, the differences in composition,<br />

pressure and temperature. 6<br />

first of these three causes. 7<br />

Elementary Theory of Diffusion only acknowledge the<br />

In Aerothermochemical problems it is advantageous to eliminate mole fraction<br />

X 1 from Eq. (2.7). Furthermore, by doing so a simplified expression is obtained.<br />

Elimination is immediately attained by keeping in mind the following relations 8<br />

Thus obtaining<br />

X 1 = M m<br />

Y 1 ,<br />

M 1<br />

(2.9)<br />

1<br />

= Y 1<br />

+ Y 2<br />

= 1 ( 1<br />

+ − 1 )<br />

Y 1 ,<br />

M m M 1 M 2 M 2 M 1 M 2<br />

(2.10)<br />

( )<br />

M1 − M 2<br />

¯f 1 = −ρD 12 ∇Y 1 + ρ D 12 Y 1 (1 − Y 1 ) ∇p<br />

M m p − D ∇T<br />

T 1<br />

T . (2.11)<br />

The first term in the right hand si<strong>de</strong> of this expression gives the diffusion flux corresponding<br />

to differences in composition. This term express Fick’s law. The second<br />

term gives the diffusion flux arising from differences in pressure. Since D 12 is always<br />

positive, formula (2.11) shows that pressure diffusion tends to carry the heavier<br />

molecules towards the higher pressures. The third term gives the diffusion flux arising<br />

from differences in temperature. Thermal diffusion coefficient D T 1 can be positive,<br />

negative or zero. Therefore, no general rules can be giving regarding the sens of this<br />

flux.<br />

Formula (2.11) shows that diffusion’s behaviour in a binary mixture of gases<br />

is <strong>de</strong>termined by the values of two coefficients: D 12 and D T 1 . Frequently D T 1 is<br />

substituted by<br />

k T =<br />

M 2 m<br />

M 1 M 2<br />

D T 1<br />

ρD 12<br />

. (2.12)<br />

Systematic measurements on diffusion coefficients of gas mixtures are not<br />

available. Therefore theoretical computations become necessary. They can be performed<br />

when knowing the interaction potential between molecules. If forces between<br />

molecules are in<strong>de</strong>pen<strong>de</strong>nt from their relative orientation, the interaction potential<br />

takes the form<br />

ϕ = ε 12 f<br />

( r<br />

σ 12<br />

)<br />

, (2.13)<br />

6 Where selective fields of forces exists, that is, fields acting with different strength over the two species<br />

of the mixture, they originate a new cause of diffusion. See Ref. [1], p. 143. Such occurs for example,<br />

when there exist ionized molecules and the mixture is submitted to the action of an electromagnetic field.<br />

7 See Ref. [5], p. 198.<br />

8 See chapter 1, pp. 12-13.

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