23rd AIAA/CEAS Aeroacoustics Conference 2017
DOI: 10.2514/6.2017-4044
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Eddy Convection in Cold and Heated Supersonic Jets

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Cited by 6 publications
(4 citation statements)
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“…In contrast to the near-nozzle region, the radial profiles at D eqA = 7, downstream of axial stations with a mean potential core region, indicate that the local convection velocity is measurably greater than the local mean velocity. These results are consistent with those reported by Ecker et al (2015) and Shea et al (2017). Bridges and Wernet (2017) analyzed convection velocities measured with time-resolved PIV and considered results from the literature for near-field hydrodynamic pressure convection velocity to interpret the findings.…”
Section: Axisymmetric Nozzle Configurationsupporting
confidence: 89%
“…In contrast to the near-nozzle region, the radial profiles at D eqA = 7, downstream of axial stations with a mean potential core region, indicate that the local convection velocity is measurably greater than the local mean velocity. These results are consistent with those reported by Ecker et al (2015) and Shea et al (2017). Bridges and Wernet (2017) analyzed convection velocities measured with time-resolved PIV and considered results from the literature for near-field hydrodynamic pressure convection velocity to interpret the findings.…”
Section: Axisymmetric Nozzle Configurationsupporting
confidence: 89%
“…The Harper-Bourne 11,12 and NASA experiments 2,8,9 have both found similar generic behavior as Tanna 1 and Tanna et al 14 measurements quantify the reduction in core length with an appropriate reduction in turbulence convection velocity (see Bridges & Wernet 2 also), which might indicate the weakness of the sound source in heated supersonic flows. Although the Ma and T R of these studies are somewhat beyond our concerns (involving supersonic source convection effects), Liu et al ( 17 , p.6) indicate that sound radiated by Mach waves is expected to enter at high frequencies at these speeds, hence the Shea/Stuber results 15,16 will be qualitatively applicable to the mild supersonic conditions under our consideration in which sound amplification due to turbulence/mean flow interaction (i.e. jet quietening effects) remain a low frequency phenomenon.…”
Section: Introductionmentioning
confidence: 74%
“…To set about showing that anyG 4 terms on the left hand side of the equation that governs ν(y 1 ,U) vanish depending on the choice of c 2 = f (U), we first integrate (13) by parts to re-write its right hand side in terms ofν(y 1 ,U) and insert the result, (12) & (15) into the i = 1 component of (7a). The latter can then be written in the following form…”
Section: Including Non-parallel Flow Effects At Lowest Order Formentioning
confidence: 99%
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