By Dougal Drysdale(auth.)
Chapter 1 fireplace technological know-how and Combustion (pages 1–34):
Chapter 2 warmth move (pages 35–82):
Chapter three Limits of Flammability and Premixed Flames (pages 83–119):
Chapter four Diffusion Flames and hearth Plumes (pages 121–179):
Chapter five regular Burning of drinks and Solids (pages 181–223):
Chapter 6 Ignition: The Initiation of Flaming Combustion (pages 225–275):
Chapter 7 unfold of Flame (pages 277–315):
Chapter eight Spontaneous Ignition inside of Solids and Smouldering Combustion (pages 317–348):
Chapter nine The Pre?Flashover Compartment fireplace (pages 349–386):
Chapter 10 The Post?Flashover Compartment fireplace (pages 387–439):
Chapter eleven Smoke: Its Formation, Composition and circulate (pages 441–474):
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Additional resources for An Introduction to Fire Dynamics, Third Edition
Water, n-hexane) will evaporate as molecules escape from the surface to form vapour. ) If the system is closed (cf. 8(a)), a state of kinetic equilibrium will be achieved when the partial pressure of the vapour above the surface reaches a level at which there is no further net evaporative loss. 13) where p o is the equilibrium vapour pressure and Lv is the latent heat of evaporation (Moore, 1972; Atkins and de Paula, 2006). 14) where E and F are constants, T is in Kelvin and p ◦ is in mm Hg. 12 (Weast, 1974/5).
R8). R7), HR4 = Hc (C3 H8 ) and HR8 = Hc (CO). 2 kJ/mol). The techniques of thermochemistry provide essential information about the amount of heat liberated during a combustion process that has gone to completion. In principle, a correction can be made if the reaction is incomplete, although the large number of products of incomplete combustion that are formed in fires make this approach cumbersome, and effectively unworkable. 2). 4), taking an appropriate value of m ˙ and assuming a value for χ to account for incomplete combustion, but an experimental method is now available by which Q˙ c can be determined.
2). The only situation where it is reasonable to ignore heat loss (at least to a first approximation) is in premixed burning, when the fuel and air are intimately mixed and the reaction rates are high, independent of diffusive or mixing processes. This is the ‘adiabatic’ model, in which it is assumed that none of the heat generated within the system is lost to the environment, thus producing the maximum theoretical rise in temperature. 14), then it is possible to estimate the adiabatic flame temperature, assuming that all the energy released is taken up by the combustion products.
An Introduction to Fire Dynamics, Third Edition by Dougal Drysdale(auth.)