2005
DOI: 10.1080/00102200590950539
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A Modified Thring–newby Scaling Criterion for Confined, Rapidly Spreading, and Unsteady Jets

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Cited by 11 publications
(2 citation statements)
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“…The scaling parameter must be preserved between the real plant and the model, and this is obtained by correcting for the variable densities in combusting systems by distorting the nozzle diameter relative to the duct diameter or the nozzle flow. This ensures that the momentum ratio of the co-flow relative to the jet in the model matches that of the reacting system (Mullinger and Jenkins 2008;Parham et al 2005). In this work, the Craya-Curtet parameter was deemed the most suitable scaling parameter (Larsson et al 2015a).…”
Section: Introductionmentioning
confidence: 99%
“…The scaling parameter must be preserved between the real plant and the model, and this is obtained by correcting for the variable densities in combusting systems by distorting the nozzle diameter relative to the duct diameter or the nozzle flow. This ensures that the momentum ratio of the co-flow relative to the jet in the model matches that of the reacting system (Mullinger and Jenkins 2008;Parham et al 2005). In this work, the Craya-Curtet parameter was deemed the most suitable scaling parameter (Larsson et al 2015a).…”
Section: Introductionmentioning
confidence: 99%
“…For this reason, detailed measurements undertaken at one condition can be considered to be broadly representative of the flow through that chamber, if undertaken at sufficiently high Re d . Parham et al (2005) used planar laser-induced fluorescence in water to assess the effects of confinement and coflow on the scalar field of the non-reacting jet emerging from this nozzle. These measurements, and those of Newbold (1997), show that true precession is present only in the first few chamber diameters.…”
Section: Introductionmentioning
confidence: 99%