By Dougal Drysdale(auth.)
Chapter 1 hearth 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 beverages 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 hearth (pages 349–386):
Chapter 10 The Post?Flashover Compartment hearth (pages 387–439):
Chapter eleven Smoke: Its Formation, Composition and circulate (pages 441–474):
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Extra resources for An Introduction to Fire Dynamics, Third Edition
16). The rate of oxidation of methane may be equated to its rate of removal by reactions b–d. , Moore (1972) or Atkins and de Paula (2006). 28 An Introduction to Fire Dynamics where the square brackets indicate concentration, and kb , kc and kd are the appropriate rate coefficients (cf. 1)). Clearly, the rate of removal of methane depends directly on the concentrations of free atoms and radicals in the reacting system. e. 16). In this respect the hydrogen atom is arguably the most important of the reactive species in the system.
Rasbash and Drysdale, 1982). 1), and can be formed even under ‘well-ventilated’ conditions, depending on the nature of the fuel. ). 1). , Rasbash, 1967; Woolley and Fardell, 1982; Gottuk and Lattimer, 2008). It is convenient to introduce here the concept of ‘equivalence ratio’, a term normally associated with premixed fuel/air mixtures. 7 The terms ‘lean’ and ‘rich’ refer to the situations where φ < 1 and φ > 1, respectively. In diffusion flames, assuming that the rate of fuel supply is known, a value can only be assigned to φ if the rate of air supply into the flame can be deduced or can be measured.
9). 1). It will be shown later that the rate at which energy is released in a fire (Q˙ c ) is the most important single factor that characterizes its behaviour (Babrauskas and Peacock, 1992). 13). 4) can still be of value when there is limited information available (see Chapter 5). 4) reveals that there are many contrib˙ c – including properties relating not only to utory factors which together determine Q the material itself (Lv and Hc ), but also to the combustion processes within the flame ˙ F and χ).
An Introduction to Fire Dynamics, Third Edition by Dougal Drysdale(auth.)