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Untitled - Aerobib - Universidad Politécnica de Madrid

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13.16. APPENDIX: APPLICATION OF PROBERT’S METHOD 333<br />

Combustion changes the droplet size distribution, preserving, obviously the<br />

maximum diameter. Figure 13.10 shows the distribution functions at the flame corresponding<br />

to the three cases studied. For comparison this figure inclu<strong>de</strong>s the distributions<br />

corresponding to the spray. Table 13.2 also gives Sauter’s diameters for both the<br />

spray and the flame.<br />

1.0<br />

0.9<br />

0.8<br />

F<br />

0.7<br />

0.6<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

ε = 1.5<br />

ε = 0.5<br />

ε = 1.0<br />

Spray<br />

Combustion<br />

0.0<br />

0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0<br />

d / d max<br />

Figure 13.10: Effect of combustion on the droplet size distribution for some values of ε.<br />

References<br />

[1] Khudyakov, G. N.: Combustion of Liquids from Free Surfaces. Isv. Acd. Sci.<br />

USER, Div. Chem. Sci., Nos. 10-11, 1945.<br />

[2] Khudyakov, G. N.: Distribution of Temperature within a Liquid Burning from<br />

a Free Surface, and Description of the Flame Formed. R.A.E. Translation no.<br />

422, 1953.<br />

[3] Spalding, B. D.: The Combustion of Liquid Fuels. Fourth Symposium (International)<br />

on Combustion, Williams and Wilkins Co., Baltimore, 1953, pp. 847-<br />

864.<br />

[4] Spalding B. D.: The Calculation of Mass Transfer Rates in Absorption, Vaporization,<br />

Con<strong>de</strong>nsation and Combustion Processes. Proceedings of the Institution<br />

of Mechanical Engineers, Vol. 168, No. 19, 1954.

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