A fundamental dimensionless number for pool fires, is proposed. Here o n and Ra~ denote a flame Schmidt number and a flame Rayleigh number. The sublayer thickness of a turbulent pool fire, 7Β’, is shown in terms of II~ to be where / is an integral scale, The fuel consumption in a turbulent pool fire
Scaling in buoyancy-driven turbulent premixed flames
β Scribed by Alexei M Khokhlov; Elaine S Oran; J.Craig Wheeler
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 735 KB
- Volume
- 105
- Category
- Article
- ISSN
- 0010-2180
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β¦ Synopsis
A scaling law is proposed that gives the steady-state turbulent flame velocity in the regime where the flame is thin compared with the largest scale of the turbulence, diffusion effects are small compared to the fluid dynamics effects, and the turbulence is driven by the Rayleigh-Taylor instability in a gravitational field. This is the regime where the fluid dynamic effects dominate diffusion. These conditions exist in premixed hydrocarbon flames approaching the flammability limits and astrophysical objects, such as supernovae. It is proposed that laboratory combustion experiments could be used to calibrate the turbulence model for supernova explosions.
π SIMILAR VOLUMES
The method of activation energy asymptotics is used to describe the behavior and characteristics of adiabatic laminar flamelets involving counterflowing reactants and products as they arise in premixed turbulent flames. For moderate and low rates of strain the results are analogous to those obtained
This work considers the applicability of different versions of the k-e hypothesis of turbulence for flame modeling. Utilizing similarity solutions, we find that the k-e hypothesis gives a finite radius for a weak axysimmetric plume above the heat source. The radius of this plume is defined as an eig
Chemical closure for premixed turbulent flames is considered, and with a small number of assumptions regarding its form, a model expression for the mean rate of product formation is obtained: (w } = C?(c }(1 -(c)) to fourth order in ((c) -1/2), with Cp a proportionality factor. Any model regardless