2019
DOI: 10.1017/jfm.2019.324
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Interaction of two-dimensional spots with a heat releasing/absorbing shock wave: linear interaction approximation results

Abstract: The canonical interaction between a two-dimensional weak Gaussian disturbance (entropy spot, density spot, weak vortex) with an exothermic/endothermic planar shock wave is studied via the Linear Interaction Approximation. To this end, a unified framework based on an extended Kovasznay decomposition that simultaneously accounts for non-acoustic density disturbances along with a poloidal-toroidal splitting of the vorticity mode and for heat-release is proposed. An extended version of Chu's definition for the ene… Show more

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Cited by 12 publications
(21 citation statements)
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“…In the supersonic case, the entropic indirect noise generation was analysed in detail by Moase, Brear & Manzie (2007) and Leyko et al. (2011), while the interaction of entropy spots with two-dimensional shock waves was studied in detail by Mahesh, Lele & Moin (1997) and Farag, Boivin & Sagaut (2019).…”
Section: Introductionmentioning
confidence: 99%
“…In the supersonic case, the entropic indirect noise generation was analysed in detail by Moase, Brear & Manzie (2007) and Leyko et al. (2011), while the interaction of entropy spots with two-dimensional shock waves was studied in detail by Mahesh, Lele & Moin (1997) and Farag, Boivin & Sagaut (2019).…”
Section: Introductionmentioning
confidence: 99%
“…The motivation was to improve descriptions of the influences of compressible turbulence on detonation propagation and, in particular, to determine how passage of a planar detonation modifies the turbulence. This work complements these fundamental studies, particularly the work of Huete et al (2013) on the interaction of detonation with density perturbations, by placing the focus on the mixture imperfections that add another type of convective perturbation (Griffond 2005;Farag, Boivin & Sagaut 2019), i.e. the local heat of combustion of the mixture.…”
Section: Introductionmentioning
confidence: 85%
“…8 Nevertheless, the sensor type would not have a noticeable effect on the results of the present study due to the absence of shocks and flow discontinuities. C T is dynamically adjusted by the shock sensor Φ as C T = 10 −⌊ 1 − 2 (1−g(Φ))⌋ , where g(Φ) = (1−Φ) 4 (1 + 4Φ) and ⌊⌋ is the Gauss bracket. 8,35 The adjustable parameters 1 and 2 are taken as 1 = 10.5 and 2 = 4.5 in the present study.…”
Section: Flux Reconstruction and Shock Capturing Schemesmentioning
confidence: 99%
“…DNS and LES of subsonic and supersonic plane channel flows with a domain size of 4 H × 2H × 4 3 H are conducted. H denotes the channel half height and is set to H = 1 in the present study.…”
Section: Problem Specificationsmentioning
confidence: 99%
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