Combustion Theory by Forman A. Williams PDF

By Forman A. Williams

ISBN-10: 0201407779

ISBN-13: 9780201407778

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Integrating this result over -Y- we find that The substitution of equation (I) into equation (4) yields equation (D-39), which-upon integration over V”-reduces to (54) Equations (51)-(54) are the integral forms of the conservation equations. 1). In the limit, the integral over d is composed of two parts, namely, integrals over each face of the slab. 1. Control volume for the derivation of interface conditions. 4. Conservation Conditions at an Interface 15 side by the subscript -. +I I + (P+ - P - ) - n + - = - Vlim +O - P-V-[(V- [itJ/ - d 4 (55) 3.

3. 17 at the lower Chapman-Jouguet point. In accordance with our earlier discussion, these numbers are typical of experimentally observed detonations but unrealistic for deflagrations. 3. 1. 1. 2 are also of general validity; only some equations and certain limits on inequalities will require modification. The expressions which must be changed are those that involve c1 explicitly, since the single parameter c1 is not sufficient to characterize the behavior of arbitrary multicomponent mixtures. We shall briefly discuss the most important complication that arises in attempting to extend our results, and then we shall summarize most of the properties of arbitrary Hugoniot curves by means of a table.

J. 0. Hirschfelder, C. F. Curtiss, and R. B. Bird, Molecular Theory of Gases and Liquids, New York: Wiley, 1954, 797-814. 4. R. A. Strehlow, Fundamentals of Combustion, Scranton, Penn. : International Textbook, 1968, 149-155. 5. Y. B. Zel’dovichand A. S. Kompaneets, TheoryofDetonation,New York: Academic Press, 1960. 68-108. 6. S. Gordon and B. J. McBride, NASA SP-273 (1971). 7. R. L. Scorah. J . Chem. Phjx 3, 425 (1935). 8. R. Becker, Z . Physik. 8, 321 (1922); Z . Elektrochem. 42,457 (1936). 9.

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Combustion Theory by Forman A. Williams

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