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Show 1.6.16 20. Andresen, P., Jacobs, A., Kleinermanns, C. and Wolfrum, J., Nineteenth Symposium (International) on Combustion, 1982, pp. 11-22. 21. Caralp, F., Tinel, C. and Loirat, IL, Combust, name 33:299-303 (1978). 22. Caralp, F. and Loirat, H., J. Chem. Res. 5:240-241 (1981). 23. Caralp, F. and Loirat, H., J. Phys. Chem. 85:2431-2432 (1981). 24. Lucas, D. and Brown, N.J., Combust. Flame 49:283-288 (1983). 25. Levy, J.M., Longwell, J.P., Sarofim, A.F., Corley, T.L., Heap, M and Tyson, T.J., in Proc. 3rd Symposium on Stationay Source Combustion, Vol. IV, EPA Report No. EPA- 600/7-79-050d, 1979, pp. 3-44. 26. Banna, S.M. and Branch, M.C., Combust. Flame 42.173-181 (1981). 27. Branch, M.C., Kee, R.J. and Miller, J.A., Combust. Sci. Techn. 29:147-165 (1982). 28. JANAF Thermochemical Tables, Stull, D.R., and Prophet, H., Project Directors, National Bureau of Standards NBS37, 2nd Ed., 1971. 29. Fujii, N., Mimyama, H., Koshi, M. and Asaba, T., Eighteenth Symposium (International) on Combustion, 1981, pp. 873-883. 30. Silver, J.A. and Kolb, C.E., Chem. Phys. Lett. 75:191-195 (1980); cf. also Silver, J.A., Optical Eng. 20:540-545 (1981). FOOTNOTE (Page 1.6.6) 1. The test section residence time tr is the sum of the characteristic mixing time tm and the time available for chemical reactions. The value of tm is not given in [4]; however, Fig. 5 of [4] indicates that tm is at most about tp/4. The resulting correction in [OH] would be less than 25% at T = 1076 K, and even smaller at higher temperatures. This correction is neglected in the present work, where tr was set equal to 2458 - 1.529 x (T in kelvin) ms. The influence of mixing has been investigated by Banna and Branch [26] and by Branch, Kee and Miller [271 |
