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Untitled - Aerobib - Universidad Politécnica de Madrid

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6.14. HYDRAZINE DECOMPOSITION FLAME 183<br />

Energy equation<br />

When mean specific heat is assumed to be constant and the influence of radicals on<br />

the energy of the mixture is neglected, the energy equation may be written<br />

( )<br />

λ dT 17<br />

m dx = q r<br />

32 − ε 2 − c p (T f − T ), (6.196)<br />

where q r is the reaction heat per gram of ammonia produced. If reduced temperatures<br />

θ = T T f<br />

and θ 0 = T 0<br />

T f<br />

(6.197)<br />

are introduced into Eq. (6.196) and taking into consi<strong>de</strong>ration the conditions at the cold<br />

boundary, θ = θ 0 , ε 2 = 0, this equation may be written<br />

where<br />

λ<br />

mc p<br />

Chemical reaction and diffusion equations<br />

The reaction equation for ammonia is<br />

dθ<br />

dx = (1 − θ 0)(1 − ε) − (1 − θ), (6.198)<br />

ε = 32<br />

17 ε 2. (6.199)<br />

m dε 2<br />

dx = w 2. (6.200)<br />

The diffusion equation corresponding to the same is given by Fick’s law and written<br />

dY 2<br />

dx = m (Y 2 − ε 2 ). (6.201)<br />

ρD 2m<br />

Coordinate x is eliminated from the above two equations through Eq. (6.198), and the<br />

following system results<br />

where<br />

and<br />

dε<br />

dθ = 32<br />

17<br />

is the Lewis-Semenov number.<br />

λ<br />

m 2 c p<br />

w 2<br />

(1 − θ 0 )(1 − ε) − (1 − θ) , (6.202)<br />

dY<br />

dθ = L Y − ε<br />

(1 − θ 0 )(1 − ε) − (1 − θ) , (6.203)<br />

Y = 32<br />

17 Y 2, (6.204)<br />

L =<br />

λ<br />

ρDc p<br />

(6.205)

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