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Experimental flammability limits and associated theoretical flame temperatures as a tool for predicting the temperature dependence of these limits
Authors:Isaac A Zlochower
Institution:1. Institut de Combustion, Aérothermique, Réactivité et Environnement (ICARE), CNRS and Université d’Orléans, 1C, av. de la Recherche Scientifique, F-45071 Orléans Cedex 02, France;2. Air Liquide, CRCD, 1 Chemin de la Porte des Loges - Les Loges-en-Josas, F-78354 Jouy-en Josas, France;1. Istituto di Ricerche sulla Combustione, CNR, Via Diocleziano 328, 80124 Napoli, Italy;2. Dipartimento di Ingegneria Chimica, dei Materiali e della Produzione Industriale, Università degli Studi di Napoli Federico II, Piazzale Tecchio 80, 80125 Napoli, Italy;1. “Ilie Mugulescu” Institute of Physical Chemistry, Romanian Academy, 202 Spl. Independentei, 060021 Bucharest, Romania;2. Physikalisch-Technische Bundesanstalt, Bundesallee 100, 38116 Braunschweig, Germany;1. KACST TIC on CCS and Mechanical Engineering Department, King Fahd University of Petroleum and Minerals, Dhahran 31261, Saudi Arabia;2. Mechanical Power Department, Faculty of Engineering, Cairo University, Giza 12613, Egypt
Abstract:The utility and limitations of adiabatic flame temperature calculations and minimum mixture energies in predicting the temperature dependence of flammability limits are explored. The limiting flame temperatures at constant pressure (1 bar) are calculated using a standard widely-used thermodynamic computer program. The computation is based on the calculated limiting flame temperature value at the reference initial temperature and the experimental limit concentration. The values recently determined in large chambers for the lower and upper flammability limits of a variety of simple organic and inorganic gases (methane, ethylene, dimethy lether, and carbon monoxide) are used as the basis for the predictions of the limiting flame temperature concept. Such thermodynamic calculations are compared with more traditional ones based on a limiting mixture energy and a constant average heat capacity of the reactant mixture. The advantages and limitations of the methods are discussed in this paper.
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