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| Content Provider | Springer Nature Link |
|---|---|
| Author | Zimont, Vladimir L. |
| Copyright Year | 2016 |
| Abstract | We formulated a paradox in the theory of turbulent premixed flame in the flamelet regime: discrepancy between the Damköhler (1940) and Shelkin (1943) estimate of the turbulence flame speed $U_{t} \sim {u}^{\prime }$ in the case of strong turbulence ( ${u}^{\prime }>>S_{L} $ ) and numerous experiments that show a strong dependence of U t on the speed of the instantaneous flame S L . We name this discrepancy the Damköhler-Shelkin paradox. The first aim of the research is to validate and clarify this estimate, which is based on intuitive considerations, as the paradox must be a statement that seems contradictory to observations but is actually true. We analysed the turbulent flame in the context of the original hyperbolic combustion equation that directly describes the leading edge of the flame, which is a locus of the Zel’dovich “leading points” controlling the speed of the turbulent flame. Analysis of the corresponding characteristic equations results in the expression for speed on the steady-state turbulent flame $U_{t} ={u}^{\prime }\sqrt {1+(S_{L} /{u}^{\prime })^{2}} $ , which is the case when ${u}^{\prime }>>S_{L} $ becomes $U_{t} \cong {u}^{\prime }$ . This result confirms and improves the Damköhler-Shelkin estimate $U_{t} \sim {u}^{\prime }$ . The second aim is to resolve the Damköhler-Shelkin paradox. We explain the discrepancy with observations by the fact that turbulent flames are transient due to insufficient residence time in the real burners to reach statistical equilibrium of wrinkle structures of the random flame surface. We consider the transient flame in the intermediate asymptotic stage when the small-scales wrinkles are in statistical equilibrium, while at the same time the large-scale wrinkles are far from equilibrium. The expressions for the flame speed and width, which we deduce using the dimensional analysis and general properties of the ransom surface, $U_{t} \sim ({u}^{\prime }S_{L})^{1/2}$ and $\delta _{t} \sim ({u}^{\prime }Lt)^{1/2}$ , show that this transient flame is in fact a turbulent mixing layer travelling with constant speed U t depending on S L , the intermediate steady propagation (ISP) flame. Qualitative estimations of the times required for the small-scale and large-scale wrinkles to reach statistical equilibrium show that the turbulent Bunsen- and V-flames correspond to the intermediated asymptotic stage, and the turbulent flames with a complete equilibrium structure of the wrinkled flamelet surface are not attainable under laboratory conditions. We present the results of numerical simulations of the impingent flames, which count in favour of the belief that these flames are also transient. |
| Starting Page | 875 |
| Ending Page | 912 |
| Page Count | 38 |
| File Format | |
| ISSN | 13866184 |
| Journal | Flow, Turbulence and Combustion |
| Volume Number | 97 |
| Issue Number | 3 |
| e-ISSN | 15731987 |
| Language | English |
| Publisher | Springer Netherlands |
| Publisher Date | 2016-02-15 |
| Publisher Place | Dordrecht |
| Access Restriction | One Nation One Subscription (ONOS) |
| Subject Keyword | Turbulent premixed flame Damköhler-Shelkin theory Hyperbolic combustion equation Engineering Fluid Dynamics Fluid- and Aerodynamics Engineering Thermodynamics, Heat and Mass Transfer Automotive Engineering |
| Content Type | Text |
| Resource Type | Article |
| Subject | Physics and Astronomy Physical and Theoretical Chemistry Chemical Engineering |
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