THE DEVELOPIì,IENT OF A HIGH PERFORMANCE
I,ASER DOPPLER VELOCII4ETER FOR FLUID MECHANICS AND ACOUSTICS RESEARCH APPLICATIONS
by
Neil Mclay WILSON. B.Tech., B.Sc.
A thesis submitted for examination for the degree of
Master of Applied Science
University of Adelaide
Mechanical Engineering Department
JuIy 1977.
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STABLI] OF CONTENTS
SUMMARY
ÀCKNOWI,EDGEMENTS NOMENCLATURE
CHAPTER 1 VEI,OCITY MEASUREMENTS IN FLUID
MECHANICS AND ACOUSTICS RES EARCII Conventional Techniques
Laser Doppler VelocimetrY
CHAPTER 2 L.D.V. METHODS, LIMITATIONS AND
ffi
1.1L.2
Page
iii i iv
10 11 14 15 18 19
I I
4
2.L
2.2 Optical HeterodYning Mode Geometries
2.2.r
2.2.2 2.2.3
Reference l4ode GeometrY
Fringe Mode GeometrY Doppler Mode GeometrY
Dístribution of Light in the Focal Volume Further Optical Considerations
2.4.L Focal Volume Size
2.4.2 Optimum Particle Specifications
2 .4 .3 SPectral Broad'ening
Directional Aliasing with Fringe Anemometers 40
2 2
3 4
2L 25
67
2.5
CHAPTER 3
CHAPTER 4
OPTICAL METHODS OF FREQUENCY BTASING
25 31 36
49 50 53 59 60 62
3.13.2 3.33.4
Mechanical SYstems
Magneto-optic Techniques Electro-optic Devices Acousto-optic Devices
4.14.1
4.r 3.4.1
3.4.2 Debye-Sear s Scattering
Bragg Diffraction
IREMENTS OF AND DESIGN PROACH
FOR A GH RES ION L.D. 77
82 86
4.I Requirements of a Laser Doppler System Optical FrequencY Biasing
Samp1e Biasing
Spectral Broadening 4.2 Frequency DemodulaÈion Methods
Frequency Domain AnaIYsis Time Domain AnalYsis
.1.2 .3
4.2.L 4.2.2
77 77 78 81 82
TABLE OF CONTENTS (CONIId)
CTIAPTER 5 OPERATION OF THE L.D.V.
Introduction
Block Diagram DÈscripti.on
Detailed Sy=tern Lìperation - Signal Processor
Analogue Unit - Ul Main Control Unit U2 Main Counter Unit U3 Buffer Storage Unit - U4
D to A Converter Unit - U5
System Specifications Applications
SUMMARY OF CONCLUSIONS
Page
89
5.r5.2 5.3
90 90 94 94 99 105 110
r14 I16
119 L24
5.3.1 s.3.2 5.3.3 s.3.4 5.3.s
5.45.5
APPENDICES
REFERENCE LIST
Logic Mnemonics
Block Diagram
Ul - Analogue Unit
U2 - Main Control Unit U3 - Main Counter Unit
V4 - Buffer Storage Unit U5 DAC Unit
Driver Circuit Acousto-optic CelI
Photographs
A1 A2 A3 A4 A5 A6 A7 B1 B2 B3
a SUMI'IARY
It is the purpose of this present study to delineate the design criteria and operating principles of a high speed, digitat laser Doppler velocimeter that is suitable for a
large nun¡ber of applications in fluid mechanics and acoustícs research.
The shortcomings of existing techniques for the measure-
ment of fLuid and surface velocities are discussed and the
advantages of laser Doppler systems are investigated'' Relevant theoretical considerations are presented, with particular
reference to the capabilities and limitations of light scatter- ing techniques. A comprehensive review cf the currently
available methods for optical frequency biasing forms the basis for the development of a high diffraction efficiency acousto-optic ceIl. The essential and desirable characteris- tics of a high performance LDV are established and incorporated into the design and construction of a digital signal processing
system that uses Èime domain analysis for the demodulation
of velocity and real time information. The system is shown
to offer solutions to the serious problems of directional aliasing; signal biasing; spectral broadening and signal dropout and is used with a modified Michelson interferometer to detect the surface velocity of a mechanically driven mirror.
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STATEMENT
This thesis contains no material which has been accepted for the award of
any other degree or diploma in any university and, to the best of my knowledge and belief' contains no material previously published or written by another person, except where due reference is made in the text.
l-l-1.
ACKNOWLEDGEME¡lTS
There are many people whom I wish to thank for their assistance and guidance during the course of this project.
In particularr mY supervisors' Drs. G.L. Brown and
D.A. Bies, vrere a continual source of inspiration and enthusi- astic encouragement. Their assistance, on So many occasions,
was readily forthcoming and always in a sense of helpful criticism and direction. Professor H.H. Davis initially provided the opportunity for me to do this research and
professor S.E. Luxtonr or appointment as Head of the Department' continued to provide the departmental assistance that' was so necessary for the successful completion of the work.
f{ithout the expertise and generous support of the
electronics workshop, the project would have required a signi- ficantly longer time for completion and would have produced an instrument well below the standard achieved. My particular thanks are therefore directed to Messrs. H. Bode, P. Walker
and G. Osborne of the Mechanicat Engineering Department Electronics lr7orkshop .
I am also grateful to Mr. A. Davis for the development and construction of the acousto-optic cell driver and for the assistance and advice that he willingly offered during the construction phase of the LDV.
In the latter stages of the project, Dr. c.J. Abell
gave me invaluable assistance through helpful cliscussion and suggestion and companionship through those times when all
seemed tost. For this I will always be indebted'
To Helen and my f amily r Ets always , I owe the greatest debt.
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NOMENCLATURE
constant
receiver apert,ure radius
speed of light
fringe spacing; grat.ing sPacing particle diameter
incident, scattered light beam unit vectors
,rth otd"t scattered light beam unit vector (Fig'13) frequency; focal length of a lens
acoustic frequencY bias frequency Doppler frequencY
frequency of incident, scattered light beam modulating frequencY
frequency of ,rth otd"r diffracted beam laser frequency
Landé g factor
height of acoustic beam; Planckrs constant intensity functions
quantum number
incident., scattered wave vectors; incident, scattered photon momentum vectors
length of focal r,'olume; Iength of laser cavity;
solenoid length.
focat volume dimension (Fig.L2) ¡ quantum number.
effective probe length molecular mean free Path
minimum probe length
total angular momentum quantum number
diffracted order; no. of particles; percentage error; no. of turns.
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NOMENCLATURE (Cont'd)
P
Pti P>t
phase retardation; elasto-optic coefficient' (79') probabilities
r pinhole radius; disc radius s Laplacian oPerator
srs'ts'rts'rts', dimensions (Fig.8) t time; focal volume thickness
v velocitY
r" acoustic velocitY
v- particle velocitY vector
;p
vf. fluid velocitY; fringe velocitY r{ beam width
*r r*r- dimensions (Fig.8)
A
D
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EP E ,
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(a) -
F H
I ro re n
receiving optics aPerture
e-1 diameter of unfocused laser beam intensities of the two incident beams incident, scattered beam intensities
intensity at the centre, âE a point p in the focal
volume.
Gaussian F number
magnetic field intensitY coil current
unattenuated laser intensitY
scattered beam intensity at an angle 0
Bessel ftn.
propogation constant of sound waves; Cunningham const.
incident phonon \^lave vector.
scattering coef f icient
J
K ruêK
Ks
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M N
NOÌ\îENCLATURE (Cont I d)
P
orbital angular momentum vector.
figure of meriti constant.
no. of wavefronts; Avogadrors no. i no. of no. of scattering Part.icles.
hydrostatic pressure acoustic power
gas constant
receiver distance from scattering volume spin angular momentum vector.
absolute temperature; measurement interval.
mean velocity
size of the focal volume acoustic beam width
const
t-
orßr'Y-
ß- ô-
angular notation modulation index
radius of beam waist
radius of scattered beam waist error due to Particle inertia refractive index; viscositY constant
angle of incidence Bragg angle
,rth otd.r diffracÈion angle.
optical wavelength
incident, scattered wavelengths.
nett magnetic moment vector Bohr magneton.
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vf..
cycles.
Np
P
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NOMENCLATURtr (Contrd)
kinematic viscosity laser frequency density
particle, f1uid. densitY minimum time of flight
angle of inclination of Yp; phase angle
incident, scattered wave functions.
angular frequencY.
angular Doppler frequencY
incident, scattered beam angular frequencies
maximum angular turbulence frequency.
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AO K
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dimension (Fig. 8)
induced change in atomic energy leve1s.
Iaser cavity half width
Doppler spectral broadenitg; Doppler frequency
He-Ne laser half line width
half the length of the focal volume (Fi9.8) ' particle Brownian motion
fringe separation
Zeeman frequencY shift
solid angle subtended by receiving aperture' geometric constant
acoustic wavelength.
solid angle of accePtance.
var.
deviation.
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