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THESIS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY in
THERMO AND FLUID DYNAMICS
Turbulence Measurements in a Natural Convection Boundary Layer and a Swirling Jet
Division of Fluid Dynamics
Department of Applied Mechanics
CHALMERS UNIVERSITY OF TECHNOLOGY
Göteborg, Sweden, 2010
Turbulence Measurements in a Natural Convection Boundary Layer and a Swirling Jet ABOLFAZL SHIRI
© ABOLFAZL SHIRI, 2010
Doktorsavhandling vid Chalmers tekniska högskola ISBN: 978-91-7385-367-5 ISSN: 0346-718X Ny serie nr: 3048
Division of Fluid Dynamics Department of Applied Mechanics Chalmers University of Technology SE-412 96 Göteborg Sweden Telephone +46 31 772 1000
This document was typeset using LATEX.
Printed at Chalmers Reproservice Göteborg, Sweden 2010
To Maryam and Arvin
Turbulence Measurements in a Natural Convection Boundary Layer and a Swirling Jet
Abolfazl Shiri [email protected]
Chalmers University of Technology Department of Applied Mechanics, Division of Fluid Dynamics
SE-412 96 Göteborg, Sweden Thesis supervisor: Professor William K. George
Abstract Two sets of experimental measurement were carried out on an axisymmetric swirling jet flow and a natural convection boundary layer. In the first experiment, the far field of an incompress- ible swirling jet, discharged into a quiescent ambient has been studied using laser Doppler anemometry. The effect of low to moderate swirl (below vortex breakdown) was studied by measuring velocity profiles of the mean and fluctuating streamwise, radial and azimuthal ve- locity components at different streamwise locations up to 50 jet exit diameters. The scaled velocity and turbulence intensity profiles, centerline decay and growth rates for two swirling jets with the strength of (S = 0.15 and 0.25) have been compared to those obtained in the same facility without swirl (S = 0). Like the previous observations for the near jet, there was no observable effect on the properly scaled far jet for the S = 0.15 case. For the S = 0.25 case, the only statistically significant effect was a shift in the virtual origin. The results were in excellent agreement with the equilibrium similarity theory of Ewing  in which the mean azimuthal component of velocity falls off as the inverse square of the downstream distance. By contrast, the mean streamwise velocity and turbulence intensities fall off with the inverse of the down- stream distance. As a consequence, the mean azimuthal equation uncouples from the rest, so the asymptotic swirling jet behaves like the non-swirling jet. The swirl is also shown to have a negligible effect on the overall Reynolds normal and shear stress balances.
Measurements are also presented for the boundary layer flow of air along a heated verti- cal cylinder. The flow was entirely driven by natural convection: there was no co-flow. The cylinder was 4.5 m in height, had a diameter of 0.15 m, and was maintained at a tempera- ture of 70◦C (approximately 40◦C above ambient). The cylinder was heated by water flowing through it, and mounted inside a 1.2 m in diameter cylindrical tunnel through which the am- bient flow could be controlled. Detailed measurements of temperature and velocity statistics were taken at heights of 1.5 m, 3m , 4 m height, the latter corresponding to a Rayleigh number based on length, Ra = gβ∆Tx4/αν ≈ 1.7 × 1011. Two-component burst-mode LDA was used for measuring the instantaneous velocity, while the fluctuating temperature was measured si- multaneously using 1-micron platinum wire. Arrays of thermocouples were used to monitor the ambient and wall conditions, as well as the mean profile. Particular attention was given to the buoyancy and momentum differential and integral equations in order to evaluate the resid- ual effects of stratification and co-flow. The strong temperature gradients and end conduction effects on the temperature probes adversely affected unsteady temperature results, as did the development with increasing height of the flow between the concentric cylinders.
Keywords: Jet, swirl, natural convection, turbulent boundary layers, vertical cylinder, high Rayleigh number, cold-wire thermometry, constant current bridge, laser Doppler anemometry.
First and foremost I would like to express my deepest gratitude to Professor William K. George. I feel myself lucky, not only to have him as a great supervisor but also privileged to be friend with him. His encouragement, enthusiasm and motivation along with extraordinary pedagog- ical skills are the source of inspiration for all of his students. When I started working with him, I did not expect the life as a Ph.D. student to be both fun and educational. The times spent with him, either traveling or working on my thesis on his boat, were unique experiences in my life. I also appreciate his effort at trying to provide the best environment for his students despite all the problems. It is a great feeling be a member of his TRL family.
I wish to thank my co-supervisor Professor Gunnar T. Johansson for all the helpful white- board discussions and criticism. His office door was always open (even in the latest time of the day) for an urgent rescue.
I would also like to thank Professor Jonathan Naughton for the help and guidance on the swirling jet project. His encouragement and inspiration was a valuable gift at the beginning of my study. I learnt a lot from him both in the subject of our research and his experience in life and work. I also appreciate his hospitality during the visit from university of Wyoming.
I enjoyed every moment of these years working amongst my close friends in the Turbulence Research Lab. group. Maja Wänström , Murat Tutkun, Carlos Arroyo, Clara Velte and Lars- Uno Axelsson, I thank you all for the great company and generous helps. I am also grateful for all the help and supports from Dr. Peter Johansson. His technical insight made working in the lab. much easier.
The natural convection project wouldn’t have started without all the effort made by Pro- fessor Rolf Karlsson. I had just a brief chance to meet him but his legacy remained with us through out the work.
I loved the tradition of daily “fika” breaks, chatting with the nice people in the department and enjoying a piece of cake or two. Thanks to all my friends in the Department of Applied Mechanics, especially Mohammad and Pirouz for making the working environment more tol- erable.
Special thanks to Lars Jernqvist for all the technical supports and last minute rescues. The project could not be progressive without his skilled provision and handiwork.
I would like to express my appreciation to Ulla Lindberg Thieme and Monica Vargman for helping me out with all sorts of paperwork and their supportive attitude.
I can not thank enough my wife, Maryam for her unconditional love and support through out all these years. I certainly could not be able to carry on with my goals and dreams without her patience and encouragement. I am also thankful to Arvin, my son, for all the joy and fun he has brought into our life. He made the final days of my Ph.D. less stressful with his rejoice.
Last but not least I am grateful to my parents who were my first teachers and without their love and encouragement I don’t think I could have succeeded.
Feb. 19th, 2010 Göteborg, Sweden
A,Bu, C growth rate constants for self-preserving axisymmetric jet Aw wire cross-sectional area Cw specific heat of wire material Cp specific heat of fluid at constant pressure Cv specific heat of fluid at constant volume D nozzle exit diameter Fo kinematic wall heat flux =
qw ρ Cp
Gθ axial component of angular momentum flux L axial length scale Mx axial momentum flux Neff number of effectively independent samples R cylinder radius; gas constant T temperature U, V,W mean axial, radial and tangential velocity components in the flow, respectively U0 average exit axial velocity of jet
U+ velocity inner variable = Uu∗
c speed of sound d wire diameter e internal energy fi vector of body force g gravitational acceleration h enthalpy; convection heat transfer coefficient k kinetic energy mx mass flux of jet in axial direction p pressure qw wall heat flux t time ; fluctuating temperature u, v, w fluctuating axial radial and azimuthal velocity component, respectively u∗ friction velocity = (τw/ρ)
x, r, θ cylindrical coordinate system xo virtual origin for self-preserving axisymmetric jet y+ inner variable =y u∗ν
α thermal diffusivity = κρCp β volumetric thermal expansion coefficient δ1/2 jet half-width
δT temperature boundary layer thickness δU velocity boundary layer thickness δij Kronecker delta ǫ dissipation of turbulent kinetic energy Φ viscous dissipation function ǫ2ψN relative statistical error of estimator ψN εν viscous dissipation η normalized radial coordinate in the momentum integral ℓ wire length κ thermal conductivity µ viscosity ν kinematic viscosity =µ/ρ ρ density σ Stefan-Boltzman constant τ temporal separation
τw wall shear stress =µ (
Grx Grashof number = gβ∆Tx3
Hx the H-number = gβFox4
M Mach number =Uc Nux Nusselt number =
hx κ =
Pr Prandtl number = να Re Reynold