posted on 2012-10-23, 13:02authored byKris Midgley
Low-emissions combustor design is crucially important to gas turbine engine
manufacturers. Unfortunately, many designs are susceptible to unsteady oscillations that
can result in structural fatigue and increased noise. Computational approaches that
resolve flow unsteadiness, for example Large Eddy Simulation (LES), are being explored
as one avenue to help understand such phenomena. However, in order to quantifY the
accuracy of LES predictions, benchmark validation data in suitably chosen test cases are
required. Comprehensive experimental data covering both time-averaged and timeresolved
features are currently scarce. It was the aim of this thesis, therefore, to provide
such data .in a configuration representing the near-field of a typical gas turbine fuel
injector. It was decided to focus on the fuel injector since many unsteady events are
believed to originate because of the transient interactions between the fuel injector flow
and the main combustor flow. A radial fed two-stream fuel injector, based on a preexisting
industrial gas-turbine Turbomeca design was used, since this geometry was
known to be susceptible to unsteadiness. The fuel injector was investigated under
isothermal conditions to place emphasis on the fluid mechanical behaviour of the fuel
injector, including detailed capture of any unsteady phenomena present. Light Sheet Imaging (LSI) systems were used as the primary experimental technique to
provide high quality spatially and temporally resolved instantaneous velocity and scalar
field information in 2D planes (using ParticieImage Velocimetry (PIV) and Planar LaserInduced
Fluorescence (PUF) techniques). Several methods were employed to extract
information quantifYing the flow unsteadiness and improve visualisation of timedependent
large-scale turbulent structures. Proper Orthogonal Decomposition (POD)
analysis enabled clear identification of the dominant modes of energy containing
structures. The results indicated that periodic high-energy containing vortex structures
occurred in the swirl stream shear layer, emerging from the fuel injector. These formed a
two-strong two-weak rotating vortex pattern which propagated down the main duct flow
path. The formation of these vortices was found to be a function of the swirl number and
originated due to an interaction between the forward moving swirl flow and the furthest
upstream penetration point ofthe recirculation zone present in the main duct flow. Dependent on the magnitude of the swirl number (influencing the swirl stream cone
angle) and the geometry of the fuel injector, the vortex formation point was sometimes
found inside the fuel injector itself. If the vortices originated inside the fuel injector they
appeared much more coherent in space and time and of higher energy. A second
unsteady high energy containing phenomenon was also identified, namely a Precessing
Vortex Core (PVC), which was damped out if the fuel injector contained a central jet.
The dynamics of the PVC interacted with the dynamics of the swirl stream shear layer
vortices to reduce there strength. Transient scalar measurements indicated that there was
a clear connection between the unsteady vortex pattern and the rate of mixing, resulting
in bursts of high heat release and is therefore identified as one source of combustor
oscillations. Future fuel injector designs need to pay close attention to these unsteady
features in selecting swirl number and internal geometry parameters.
History
School
Aeronautical, Automotive, Chemical and Materials Engineering