Abstract
Swirl-stabilised combustion is one of the most widely used techniques for flame stabilisation, uses ranging from gas turbine combustors to pulverised coal-fired power stations. In gas turbines, lean premixed systems are of especial importance, giving the ability to produce low NOx systems coupled with wide stability limits. The common element is the swirl burner, which depends on the generation of an aerodynamically formed central recirculation zone (CRZ) and which serves to recycle heat and active chemical species to the root of the flame as well as providing low-velocity regions where the flame speed can match the local flow velocity. Enhanced mixing in and around the CRZ is another beneficial feature. The structure of the CRZ and hence that of the associated flames, stabilisation and mixing processes have shown to be extremely complex, three-dimensional and time dependent. The characteristics of the CRZ depend very strongly on the level of swirl (swirl number), burner configuration, type of flow expansion, Reynolds number (i.e. flowrate) and equivalence ratio. Although numerical methods have had some success when compared to experimental results, the models still have difficulties at medium to high swirl levels, with complex geometries and varied equivalence ratios. This study thus focuses on experimental results obtained to characterise the CRZ formed under varied combustion conditions with different geometries and some variation of swirl number in a generic swirl burner. CRZ behaviour has similarities to the equivalent isothermal state, but is strongly dependent on equivalence ratio, with interesting effects occurring with a high-velocity fuel injector. Partial premixing and combustion cause more substantive changes to the CRZ than pure diffusive combustion.
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Abbreviations
- A e :
-
Tangential inlet area [m2]
- CRZ:
-
Central recirculation zone
- D :
-
Exit diameter of burner
- Dcrz:
-
Maximum diameter of CRZ
- HMFR:
-
High-momentum flow region
- JMR:
-
Jet momentum ratio, fuel jet axial momentum relative to that in the surrounding annulus [−]
- L:
-
Length of CRZ beyond burner exit, [m]
- NUcrz:
-
Uaxrev/Uannulus [−]
- PVC:
-
Precessing vortex core
- Re :
-
Reynolds number. Here defined using average exhaust velocity and gas kinematic viscosity under isothermal conditions [−]
- r e :
-
Exit radius of the burner [m]
- r i :
-
Radius upon which the tangential inlet jets fire [m]
- S*:
-
Swirl number modified by combustion (Valera-Medina 2009a)
- S g :
-
Geometrical swirl number (Syred 2006)
- Uannulus:
-
Average axial velocity in the annulus surrounding the fuel injector [m/s]
- Uaxrev:
-
Average axial velocity in CRZ derived from PIV measurements [m/s]
- φ p :
-
Premixed equivalence ratio
- φ t :
-
Overall equivalence ratio
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Acknowledgments
Agustin Valera-Medina gratefully acknowledges the receipt of a scholarship from the Mexican Government (CONACYT) to carry out his PhD programme at Cardiff University and for the assistance of Malcom Seaborne during the set-up of the experiments.
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Valera-Medina, A., Syred, N., Kay, P. et al. Central recirculation zone analysis in an unconfined tangential swirl burner with varying degrees of premixing. Exp Fluids 50, 1611–1623 (2011). https://doi.org/10.1007/s00348-010-1017-7
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DOI: https://doi.org/10.1007/s00348-010-1017-7