TY - JOUR
T1 - Numerical study of flame/vortex interactions in 2-D trapped vortex combustor
AU - Mishra, Debi Prasad
AU - Sudharshan, Renganathan
AU - Ezhil Kumar, Perumal Kumaresan
PY - 2014
Y1 - 2014
N2 - The interactions between flame and vortex in a 2-D trapped vortex combustor are investigated by simulating the Reynolds averaged Navier-Stokes equations, for the following five cases: (1) non-reacting (base) case, (2) post-vortex ignition without premixing, (3) post-vortex ignition with premixing, (4) pre-vortex ignition without premixing, and (5) pre-vortex ignition with premixing. For the post-vortex ignition without premixing case, the reactants are mixed well in the cavity resulting in a stable C shaped flame along the vortex edge. Further, there is insignificant change in the vorticity due to chemical reactions. In contrast, for the pre-vortex ignition case (no premixing); the flame gets stabilized at the interface of two counter rotating vortices resulting in reduced reaction rates. There is a noticeable change in the location and size of the primary vortex as compared to case (2). When the mainstream air is premixed with fuel, there is a further reduction in the reaction rates and thus structure of cavity flame gets altered significantly for case (5). Pilot flame established for cases (2) and (3) are well shielded from main flow and hence the flame structure and reaction rates do not change appreciably. Hence, it is expected that cases (2) and (3) can perform well over a wide range of operating conditions.
AB - The interactions between flame and vortex in a 2-D trapped vortex combustor are investigated by simulating the Reynolds averaged Navier-Stokes equations, for the following five cases: (1) non-reacting (base) case, (2) post-vortex ignition without premixing, (3) post-vortex ignition with premixing, (4) pre-vortex ignition without premixing, and (5) pre-vortex ignition with premixing. For the post-vortex ignition without premixing case, the reactants are mixed well in the cavity resulting in a stable C shaped flame along the vortex edge. Further, there is insignificant change in the vorticity due to chemical reactions. In contrast, for the pre-vortex ignition case (no premixing); the flame gets stabilized at the interface of two counter rotating vortices resulting in reduced reaction rates. There is a noticeable change in the location and size of the primary vortex as compared to case (2). When the mainstream air is premixed with fuel, there is a further reduction in the reaction rates and thus structure of cavity flame gets altered significantly for case (5). Pilot flame established for cases (2) and (3) are well shielded from main flow and hence the flame structure and reaction rates do not change appreciably. Hence, it is expected that cases (2) and (3) can perform well over a wide range of operating conditions.
UR - http://www.scopus.com/inward/record.url?scp=84916883314&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84916883314&partnerID=8YFLogxK
U2 - 10.2298/TSCI111006162M
DO - 10.2298/TSCI111006162M
M3 - Article
AN - SCOPUS:84916883314
SN - 0354-9836
VL - 18
SP - 1373
EP - 1387
JO - Thermal Science
JF - Thermal Science
IS - 4
ER -