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Untitled - Aerobib - Universidad Politécnica de Madrid

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266 CHAPTER 11. SIMILARITY IN COMBUSTION. APPLICATIONS<br />

The interpretation of the meaning of Damköhler two parameters is simple. The<br />

first is a measurement of the relationship between the mean mechanical time required<br />

by a particle to travel the characteristic lenght l 0 at the characteristic velocity v 0 and<br />

the time required by the chemical reaction of the mixture to take place. The second<br />

parameter of Damköhler is a measure of the relationship between the heat produced<br />

by unity of mixture when burning at constant pressure and the heat contained by the<br />

same at characteristic temperature T 0 .<br />

It should be noted that in the non-stationary processes a additional parameter<br />

appears, Strouhal number, which originates from the time <strong>de</strong>rivatives ∂/∂t of the<br />

equations of motions. Likewise, if the mass forces are present as occurs in the phenomena<br />

of free convection, then another dimensionless parameter appears, due to the<br />

gravity terms of the equations, which originates the Frou<strong>de</strong> number.<br />

Finally, when the number of species and chemical reaction is increased, the<br />

number of the Damköhler parameters (of both kinds time and heat) increases as well.<br />

In technical literature we frequently find other parameter which are combinations<br />

of the above mentioned. Por example, occasionally Prandtl number is substituted<br />

by Peclet number, which is a product of the numbers of Reynolds and Prandtl<br />

Pe = Pr · Re = ρ 0v 0 l 0 c p0<br />

λ 0<br />

. (11.26)<br />

Likewise, the Schmidt number is replaced by the Lewis-Semenov number which is<br />

obtained as follows<br />

L = Pr<br />

Sc = ρ 0D 0 c p0<br />

, (11.27)<br />

λ 0<br />

used specially in combustion processes as seen in Chap. 6.<br />

The advantage of utilizing the Peclet and Lewis-Semenov numbers in combustion<br />

phenomena is based on the fact that the conductivity and diffusion coefficients<br />

appear explicity in their expressions. Such coefficients are the ones of interest in these<br />

processes in which the influence of the viscosity coefficient is negligible in many<br />

cases, as said in Chap. 5.<br />

We shall now see some practical applications of this theory.<br />

11.3 Scaling of rockets<br />

The problem of the scaling of rockets has a great practical interest since its solutions<br />

would allow the prediction of the behavior of the rockets after tests ma<strong>de</strong> with reduced<br />

scale mo<strong>de</strong>ls.

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