Reynolds stress statistics in the near nozzle region of coaxial swirling jets

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Abstract

Particle image velocimetry (PIV) was used to obtain the mean axial velocity , the mean radial velocity and the Reynolds stress statistics in an isothermal flow formed by discharging a central jet in an annular stream of swirling air flow. This is a typical geometry used in swirl-stabilised burners, where the central jet is the fuel. The flow Reynolds number was 29000, based on the area-averaged velocity of 8.46 m/s at the exit and the diameter of swirling co-flow of 50.8 mm. Three swirl numbers, S, of 0.3, 0.58, and 1.07 of the annular swirling stream were considered. The effects of the swirl number on the behaviours of the Reynolds stresses, and their gradients, which appear in the Reynolds-averaged Navier-Stokes (RANS) equations are analysed. The results show pronounced asymmetry in the mean and the fluctuating quantities for all swirl numbers. The flow asymmetricity is found to be related to the radial velocity fluctuations. It was postulated that for swirling flows with constant Reynolds number the change in the flow swirl number only, does not necessary result in increase of turbulent intensity. An 'effective' turbulent viscosity was shown to be independent of the flow swirl number for constant Reynolds number.
LanguageEnglish
Pages332-349
JournalInternational Journal of Hydromechatronics
Volume1
Issue number3
DOIs
Publication statusPublished - 20 Sep 2018

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swirling
Reynolds stress
nozzles
statistics
Reynolds number
radial velocity
isothermal flow
burners
air flow
particle image velocimetry
Navier-Stokes equation
asymmetry
viscosity
gradients
geometry

Cite this

@article{b82362997ae54615a825731c0af70960,
title = "Reynolds stress statistics in the near nozzle region of coaxial swirling jets",
abstract = "Particle image velocimetry (PIV) was used to obtain the mean axial velocity , the mean radial velocity and the Reynolds stress statistics in an isothermal flow formed by discharging a central jet in an annular stream of swirling air flow. This is a typical geometry used in swirl-stabilised burners, where the central jet is the fuel. The flow Reynolds number was 29000, based on the area-averaged velocity of 8.46 m/s at the exit and the diameter of swirling co-flow of 50.8 mm. Three swirl numbers, S, of 0.3, 0.58, and 1.07 of the annular swirling stream were considered. The effects of the swirl number on the behaviours of the Reynolds stresses, and their gradients, which appear in the Reynolds-averaged Navier-Stokes (RANS) equations are analysed. The results show pronounced asymmetry in the mean and the fluctuating quantities for all swirl numbers. The flow asymmetricity is found to be related to the radial velocity fluctuations. It was postulated that for swirling flows with constant Reynolds number the change in the flow swirl number only, does not necessary result in increase of turbulent intensity. An 'effective' turbulent viscosity was shown to be independent of the flow swirl number for constant Reynolds number.",
keywords = "Reynolds stress, swirling jet, RANS, coaxial",
author = "Viacheslav Stetsyuk and {Chai Chee Kiong}, John",
year = "2018",
month = "9",
day = "20",
doi = "10.1504/IJHM.2018.10016315",
language = "English",
volume = "1",
pages = "332--349",
journal = "International Journal of Hydromechatronics",
issn = "2515-0472",
publisher = "Inderscience Publishers",
number = "3",

}

TY - JOUR

T1 - Reynolds stress statistics in the near nozzle region of coaxial swirling jets

AU - Stetsyuk, Viacheslav

AU - Chai Chee Kiong, John

PY - 2018/9/20

Y1 - 2018/9/20

N2 - Particle image velocimetry (PIV) was used to obtain the mean axial velocity , the mean radial velocity and the Reynolds stress statistics in an isothermal flow formed by discharging a central jet in an annular stream of swirling air flow. This is a typical geometry used in swirl-stabilised burners, where the central jet is the fuel. The flow Reynolds number was 29000, based on the area-averaged velocity of 8.46 m/s at the exit and the diameter of swirling co-flow of 50.8 mm. Three swirl numbers, S, of 0.3, 0.58, and 1.07 of the annular swirling stream were considered. The effects of the swirl number on the behaviours of the Reynolds stresses, and their gradients, which appear in the Reynolds-averaged Navier-Stokes (RANS) equations are analysed. The results show pronounced asymmetry in the mean and the fluctuating quantities for all swirl numbers. The flow asymmetricity is found to be related to the radial velocity fluctuations. It was postulated that for swirling flows with constant Reynolds number the change in the flow swirl number only, does not necessary result in increase of turbulent intensity. An 'effective' turbulent viscosity was shown to be independent of the flow swirl number for constant Reynolds number.

AB - Particle image velocimetry (PIV) was used to obtain the mean axial velocity , the mean radial velocity and the Reynolds stress statistics in an isothermal flow formed by discharging a central jet in an annular stream of swirling air flow. This is a typical geometry used in swirl-stabilised burners, where the central jet is the fuel. The flow Reynolds number was 29000, based on the area-averaged velocity of 8.46 m/s at the exit and the diameter of swirling co-flow of 50.8 mm. Three swirl numbers, S, of 0.3, 0.58, and 1.07 of the annular swirling stream were considered. The effects of the swirl number on the behaviours of the Reynolds stresses, and their gradients, which appear in the Reynolds-averaged Navier-Stokes (RANS) equations are analysed. The results show pronounced asymmetry in the mean and the fluctuating quantities for all swirl numbers. The flow asymmetricity is found to be related to the radial velocity fluctuations. It was postulated that for swirling flows with constant Reynolds number the change in the flow swirl number only, does not necessary result in increase of turbulent intensity. An 'effective' turbulent viscosity was shown to be independent of the flow swirl number for constant Reynolds number.

KW - Reynolds stress

KW - swirling jet

KW - RANS

KW - coaxial

U2 - 10.1504/IJHM.2018.10016315

DO - 10.1504/IJHM.2018.10016315

M3 - Article

VL - 1

SP - 332

EP - 349

JO - International Journal of Hydromechatronics

T2 - International Journal of Hydromechatronics

JF - International Journal of Hydromechatronics

SN - 2515-0472

IS - 3

ER -