Damon Honnery

Dr. Damon Honnery

Department of Mechanical and Aerospace Engineering, Monash University, Melbourne VIC 3145, Australia

Research Focus & Metrics

Academic Career Length

40Years (1987-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 January 2012 in Renewable and Sustainable Energy Reviews
Verified
Journal Article
Closed access
Patrick MoriartyPatrick Moriarty
Patrick Moriarty
DHDamon Honnery
Damon Honnery

1 June 2016 in Energy Policy
Verified
Journal Article
Closed access
Patrick MoriartyPatrick Moriarty
Patrick Moriarty
DHDamon Honnery
Damon Honnery

1 January 2009 in International Journal of Hydrogen Energy
Verified
Journal Article
Closed access
Patrick MoriartyPatrick Moriarty
Patrick Moriarty
DHDamon Honnery
Damon Honnery

3 December 2011 in Experiments in Fluids
Verified
Journal Article
Closed access
PDF file
DDDaniel Duke
Daniel Duke
JSJulio Soria
Julio Soria
DHDamon Honnery
Damon Honnery

1 August 2007 in International Journal of Hydrogen Energy
Verified
Journal Article
Closed access
Patrick MoriartyPatrick Moriarty
Patrick Moriarty
DHDamon Honnery
Damon Honnery

8 May 2014 in Journal of Fluid Mechanics
Verified
Journal Article
Closed access
PDF file
DEDaniel Edgington-Mitchell
Daniel Edgington-Mitchell
KOKILIAN OBERLEITHNER
KILIAN OBERLEITHNER
DHDamon Honnery
Damon Honnery
JSJulio Soria
Julio Soria
The structure of a screeching axisymmetric jet in the helical C mode at a nozzle pressure ratio of 3.4 issuing from a convergent nozzle is studied using high-resolution particle image velocimetry. Proper orthogonal decomposition (POD) is used to extract the dominant coherent structures within the jet. The first two modes produced by the POD are used to reconstruct a phase-averaged data sequence. A triple decomposition into mean, coherent and random velocity components is performed. The embedded shock structures within the jet are shown to strongly modulate the coherent axial stresses within the shear layer and to weakly modulate the random axial stresses. Analysis of the third and fourth moments of the velocity probability density function is used as an indicator of possible regions of shock–vortex interaction and thus screech tone generation. Peaks of kurtosis (flatness) occur at the second, third and fourth shock–boundary intersection points, with the radial position shifting towards the centreline with increasing downstream distance. Analysis of the coherent component of vorticity shows that the largest fluctuations in coherent vorticity occur at the high-speed side of the shear layer in an area extending from the second to the fourth shock cell. With reference to prior literature, the argument is made that it is this increased magnitude of coherent vorticity fluctuation that is the primary factor in the determination of which shock cells act as dominant screech sources.