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For Reaction H.1, we may define an equilibrium constant with the follow-ing relation: H.2 The brackets denote the volume concentrations of the enclosed species... 618 Modeling of Combust

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Appendix H

Equilibrium Primer

Consider a general reaction:

or equivalently

(H.1)

Here, j is an index from 1 to m reactants, r j refers to the number of moles

of the jth reactant, R j is the jth reactant, the double-headed arrow (↔) means that both the forward and reverse reactions occur (typically at different rates),

k is an index from 1 to n products, p k is the number of moles of the kth product,

and P k is the kth product

For Reaction H.1, we may define an equilibrium constant with the follow-ing relation:

(H.2)

The brackets denote the volume concentrations of the enclosed species If

we wish to express K eq in terms of mole fraction rather than concentration for gases, then, using the ideal gas law, we obtain

(H.3)

r1R1+r2R2+ ↔$ p1 1P +p2 2P +$

j

m

k k k

n

R

∑ ↔∑

P

K

k

= ⎡⎣ ⎤⎦ ⎡⎣ ⎤⎦

⎡⎣ ⎤⎦

P

1 2

1 2

1 2

1 2

$

$

pp k n

j r j m

k

j

=

=

1

1

R

RT

s s r r

S s S s r

=⎛

⎝⎜

⎠⎟

+ + − − −

1 2 1 2

1 1 2 2 1 1

$ $

$

R R

S

R

2 2

1

1

r

s r

s k n

r j m

P RT

y y

k

k j

$=⎛

⎝⎜

⎠⎟

=

=

© 2006 by Taylor & Francis Group, LLC

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618 Modeling of Combustion Systems: A Practical Approach

Please note that P and R (italicized) are the pressure and universal gas

constant, while P and R (nonitalicized) refer to products and reactants, respectively

For constant-pressure systems such as combustion, we may also incorpo-rate the pressure dependence as part of the equilibrium constant, as

:

(H.4)

In either case, the equilibrium constant is defined as products over reactants

K (or K y) is a function of temperature according to an Arrhenius relation:

(H.5)

Thus, K (or K y) is only constant if the reaction temperature is constant Since temperature is in the exponential, it usually overwhelms the temperature

effects shown in Equation H.3 In particular, note that K y is neither necessarily dimensionless nor independent of pressure, except in the case that the num-ber of moles remains invariant

P

p k r k

K

y y y

p k n

r j m

k k

k j

=

P

R 1

1

b T

© 2006 by Taylor & Francis Group, LLC

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