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Untitled - Aerobib - Universidad Politécnica de Madrid

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8.3. FLAMMABILITY LIMITS 225<br />

The preceding system of equations allows an easy simplification, by using the<br />

stream function ψ, frequently applied to the problem of Fluid Mechanics.<br />

The said function is <strong>de</strong>fined by the following conditions<br />

ρ = ∂ψ<br />

∂x ,<br />

ρv = −∂ψ<br />

∂t , (8.11)<br />

through which Eq. (8.7) is i<strong>de</strong>ntically satisfied. When taking Eq. (8.11) into Eqs. (8.8)<br />

and (8.9), this system reduces to the following<br />

∂T<br />

∂t = ∂ ( ρλ ∂T<br />

∂ψ c p ∂ψ<br />

∂Y<br />

∂t = ∂ ( ρ 2 D<br />

∂ψ<br />

Thus the variable v has been eliminated.<br />

c p<br />

∂Y<br />

∂ψ<br />

)<br />

+ q c p<br />

w<br />

ρ , (8.12)<br />

)<br />

+ w ρ . (8.13)<br />

The integration of the above system has not yet been performed. However,<br />

Spalding [7] has obtained graphical solutions of Eq. (8.12) disregarding diffusion.<br />

These solutions show the existence of a critical value d cr for d un<strong>de</strong>r which the wave<br />

extinguishes, while for d > d cr it propagates in<strong>de</strong>finitely.<br />

There are some experimental observations on the evolution followed by an<br />

ignited mass before the flame establishes [8].<br />

8.3 Flammability limits<br />

The theoretical studies performed so far have shown that the combustible mixture is<br />

always capable of maintaining a flame. Experimentally, however, it has been verified<br />

that it is not so, since there are numerous mixtures which, in practise, are not able to<br />

propagate a flame, even when theory predicts otherwise.<br />

In fact, experiments disclose that when analyzing the behavior of a combustible<br />

mixture un<strong>de</strong>r pressure and temperature constant, but changing its composition, for instance<br />

a mixture of fuel and air, the flame velocity is maximum for a <strong>de</strong>finite value<br />

of the composition which is normally very close to the stoichiometric one, and it <strong>de</strong>creases<br />

for mixtures either rich or loan, up to values known as inflammability limits of<br />

the mixture, beyond which it cannot propagate a flame. Moreover the flame velocity<br />

does not vanish at the inflammability limits but it generally reaches values of a few<br />

centimeters per second. Inflammability limits <strong>de</strong>pend also on pressure and they are<br />

difficult to <strong>de</strong>termine experimentally because it is necessary to operate un<strong>de</strong>r marginal<br />

conditions, on which the experimental techniques might have an influence. Tables

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