2015
DOI: 10.1063/1.4919594
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Absolute and convective instabilities of heated coaxial jet flow

Abstract: This study investigates the inviscid, linear spatio-temporal stability of heated, compressible and incompressible coaxial jet flows. The influence of the temperature ratio and the velocity ratio between the core jet and the bypass stream on the transition from convectively to absolutely unstable flows is studied numerically. The investigation shows that for coaxial jets absolute instability can occur for considerably lower core-stream temperatures than for single jets. The reason for this modified stability ch… Show more

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Cited by 22 publications
(27 citation statements)
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“…This behaviour seems to be linked with the apparent decrease of the group velocity at the velocity perturbations maximum. Similar results have also been observed by Balestra et al (2015) in co-axial jets. Furthermore, Nichols et al (2007) observed that absolute instabilities intensified when the maximum shear aligns with the density shear in heated round jets.…”
Section: Introductionsupporting
confidence: 90%
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“…This behaviour seems to be linked with the apparent decrease of the group velocity at the velocity perturbations maximum. Similar results have also been observed by Balestra et al (2015) in co-axial jets. Furthermore, Nichols et al (2007) observed that absolute instabilities intensified when the maximum shear aligns with the density shear in heated round jets.…”
Section: Introductionsupporting
confidence: 90%
“…Velocity profiles at the chamber inlet exhibit two streams and shear layers, similarly to coaxial jets studied in the literature (Balestra et al. 2015). The main stream is caused by the heating at the jet centreline, while the secondary stream originates from the annular inlet.…”
Section: Problem and Model Descriptionsupporting
confidence: 65%
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“…Following Bassi 7 and Balestra, Gloor, and Kleiser, 48 we use the saddle point method to find solutions of the dispersion relation, i.e., D(ω, k) = 0, for the complex pair (ω 0 , k 0 ), where D(ω 0 , k 0 ) = ∂D(ω 0 , k 0 )/∂k = 0 and ∂ 2 D(ω 0 , k 0 )/∂k 2 ≠ 0. In order to investigate the behavior of changing dimensionless parameters, we consider a reference state, where We = 2, F = 4, Re = 800, α = 3 and De = 10 at z = 0.…”
Section: B Finding the Saddle Pointmentioning
confidence: 98%