Air Bubble Entrainment in Free-Surface Turbulent Shear Flows -  Hubert Chanson

Air Bubble Entrainment in Free-Surface Turbulent Shear Flows (eBook)

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1996 | 1. Auflage
348 Seiten
Elsevier Science (Verlag)
978-0-08-052689-8 (ISBN)
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This book develops an analysis of the air entrainment processes in free-surface flows. These flows are investigated as homogeneous mixtures with variable density. Several types of air-water free-surface flows are studied: plunging jet flows, open channel flows, and turbulent water jets discharging into air. Experimental observations reported by the author confirm the concept that the air-water mixture behaves as a homogeneous compressible fluid in each case. This book will be of great interest to professionals working in many fields of engineering: chemical, civil, environmental, mechanical, mining, metallurgy, and nuclear.

Key Features
* Covers new information on the air-water flow field: air bubble distributions, air-water velocity profiles, air bubble sizes and bubble-turbulence interactions
* Features new analysis is developed for each flow configuration and compared successfully with model and prototype data
* Includes over 372 references and more than 170 figures with over 60 photographs
* Presents useful information for design engineers and research-and-development scientists who require a better understanding of the fluid mechanics of air-water flows
This book develops an analysis of the air entrainment processes in free-surface flows. These flows are investigated as homogeneous mixtures with variable density. Several types of air-water free-surface flows are studied: plunging jet flows, open channel flows, and turbulent water jets discharging into air. Experimental observations reported by the author confirm the concept that the air-water mixture behaves as a homogeneous compressible fluid in each case. This book will be of great interest to professionals working in many fields of engineering: chemical, civil, environmental, mechanical, mining, metallurgy, and nuclear. Covers new information on the air-water flow field: air bubble distributions, air-water velocity profiles, air bubble sizes and bubble-turbulence interactions Features new analysis is developed for each flow configuration and compared successfully with model and prototype data Includes over 372 references and more than 170 figures with over 60 photographs Presents useful information for design engineers and research-and-development scientists who require a better understanding of the fluid mechanics of air-water flows

Front Cover 1
Air Bubble Entrainment in Free-surface Turbulent Shear Flows 4
Copyright Page 5
TABLE OF CONTENTS 8
Dédicace 6
Abstract / Résumé 16
Album of 'white water' photographs 18
Acknowledgements 22
About the author 23
List of symbols 24
Glossary 36
PART I: INTRODUCTION 56
Chapter 1. Introduction 57
1.1 Presentation 57
1.2 Applications of air-water flows 63
1.3 Bibliography 70
1.4 Structure of the monograph 71
Chapter 2. Mechanisms of air bubble entrainment 72
2.1 Introduction 72
2.2 Mechanisms of air entrainment 72
2.3 High-velocity air-water flows 76
2.4. Definition of the air-water 'free-surface' 77
2.5 Compressibility effects in high-velocity air-water flows 79
2.6 Summary 81
Chapter 3. Similitude and experimental studies 82
3.1 Introduction 82
3.2 Dimensional analysis 82
3.3 Experimental studies of high-velocity air-water flows 85
Chapter 4. Air-water gas transfer 91
4.1 Introduction 91
4.2 Basic equations 91
4.3 Bibliography 92
4.4 Interactions between air entrainment and water quality 94
PART II: PLUNGING JET ENTRAINMENT 98
Chapter 5. Plunging jet flows: presentation 99
5.1 Introduction 99
5.2 Mechanisms of air entrainment and inflow conditions 99
5.3 Air bubble diffusion 103
Chapter 6. Air entrainment by plunging jets 108
6.1 Introduction 108
6.2 Air entrainment mechanisms - quantity of entrained air 113
6.3 Flow pattern of the air-water shear region 116
6.4 Air-water flow properties in the developing flow region 117
6.5 Fully-developed air-water shear flow 123
6.6 Discussion 126
Chapter 7. Air entrainment in hydraulic jumps 128
7.1 Introduction 128
7.2 Flow patterns 133
7.3 Quantity of entrained air 134
7.4 Air bubble diffusion 138
7.5 Discussion 144
7.6 Summary 147
Chapter 8. Air entrainment in plunging jet flows: related cases and gas transfer 148
8.1 Introduction 148
8.2 Air entrainment in siphon spillways 148
8.3 Nappe flow regime 151
8.4 Air-water gas transfer 153
PART III: SELF-AERATED OPEN CHANNEL FLOWS 158
Chapter 9. Self-aerated flows - presentation 159
9.1 Introduction 159
9.2 Historical investigations 159
9.3 Structure of the air-water flow 161
9.4 Definitions 162
Chapter 10. Air entrainment in steep chute flows 165
10.1 Introduction 165
10.2 Non-aerated developing flow region 166
10.3 Uniform equilibrium flows 170
10.4 Gradually-varied flows 182
10.5 Discussion 185
Chapter 11. Air entrainment in small-slope waterways 188
11.1 Introduction 188
11.2 Developing flow region 188
11.3 Fully-developed flow region 193
11.4 Discussion 195
11.5 Summary 197
Chapter 12. Air entrainment in partially-filled conduits 199
12.1 Introduction 199
12.2 Re-analysis of existing data 201
12.3 Discussion 204
Chapter 13. Air entrainment in open channels: discussion 208
13.1 Introduction 208
13.2 Self-aeration in rough channels 208
13.3 Air-water interface area in self-aerated flows 211
13.4 Air-water gas transfer on smooth chutes 216
PART IV: HIGH-VELOCITY WATER JETS AND RELATED AIR-WATER FLOWS 220
Chapter 14. Introduction to high-velocity water jets discharging into the atmosphere and ventilated cavity flows 221
14.1 Presentation 221
14.2 Bibliography 223
14.3 Flow patterns of water jets discharging into air 223
Chapter 15. Air entrainment in high-velocity water jets 229
15.1 Introduction 229
15.2 Air bubble entrainment 229
15.3 Velocity distributions 238
15.4 Discussion 240
Chapter 16. Ventilated cavity flows 244
16.1 Presentation 244
16.2 Ventilated cavity flows 244
16.3 Discussion: related cases 253
Chapter 17. Spillway application: aeration devices 255
17.1 Introduction 255
17.2 Aeration mechanisms and flow regions 259
17.3 Downstream flow region 267
17.4 Discussion 268
PART V: SUMMARY AND CONCLUSION 270
Chapter 18. Summary: air bubble diffusion in shear flows 271
18.1 Introduction 271
18.2 Flow characteristics 273
18.3 Interactions between turbulence and air bubbles 279
18.4 Analogy with other particle/turbulence interaction phenomena 285
18.5 Summary 288
Chapter 19. Conclusion 290
19.1 Summary 290
19.2 Fundamental results 291
19.3 Air bubble diffusion 292
19.4 Air-water flow characteristics 292
19.5 Future research 293
References 294
APPENDICES 318
Appendix A. Constants and fluid properties 318
Appendix B. Unit conversions 326
Appendix C. Bubble rise velocity 329
Appendix D. Sound celerity in two-phase (gas-liquid) flow 333
Appendix E. Air bubble diffusion at plunging water jets 336
Appendix F. Characteristic parameters of a boundary layer 344
Appendix G. Air concentration distributions in self-aerated flows 348
Appendix H. Air-water flow in partially-filled pipes 359
Appendix I. Air concentration distributions in water jets discharging into the atmosphere 362
Appendix J. Jet trajectory calculations 371
Appendix K. Air bubble size distribution characteristics 378
Appendix L. Air-water flow as recounted by LEONARDO DA VINCI 382
Appendix M. Corrections 385
Index of authors 388
Subject index 394

List of symbols


A cross-section area (m2);

Aab cross-section area (m2) of air bubble in a particular direction (App. C);

AW clear-water flow cross-section area (m2);

A1,A2 constants (see App. A);

A3,A4 constants (see App. A);

A90 air-water flow cross-section area (m2) (i.e. for C < 0.90);

a specific interface area (m− l);

a1, a2 constants;

B coefficient of proportionality (see App. G);

B′ integration constant (defined by WOOD 1984) (see App. G);

B1, B2, B3 constants (see App. A);

B90 free-surface width (m) of the air-water flow (i.e. at y = Y90);

C air concentration defined as the volume of air per unit volume of air and water; it is also called void fraction;

CDS downstream dissolved gas concentration (kg/m3);

CT characteristic air concentration defined as : CT= C(y=dT) (see App. G);

CUS upstream dissolved gas concentration (kg/m3);

Cb air concentration next to a solid boundary;

Cd drag coefficient;

Ce mean air concentration in uniform equilibrium self-aerated flow;

Cgas concentration of dissolved gas in water (kg/m3);

Cmax maximum air concentration in the air bubble diffusion layer;

(Cmax)o initial maximum air concentration;

(Cmax)I maximum air concentration at inflow;

Cmean mean air concentration defined in terms of 90%-air content :
(1 - Cmean) * Y90 = d in two-dimensional flow down a rectangular cross-section channel;
mean=1A90*∫0Y90∫C*dz*dy in partially-filled pipes and channels of irregular cross-section;

(Cmean)cl mean air concentration on the channel centreline;

(Cmean)max maximum mean air concentration along a chute;

(Cmean)1 mean air concentration at the inflow of pre-entrained hydraulic jump;

Co initial air content;

Cp specific heat at constant pressure (J/kg.K) (see App. A);

Csat gas saturation concentration in water (kg/m3) (see App. A);

Csed mean volumetric sediment concentration;

Csound sound celerity (m/s) (see App. A and D);

Cv specific heat at constant volume (J/kg.K) (see App. A);

C* mean air concentration at x = 0 in self-aerated flow (Chap. 10);

Chl chlorinity;

ch chord length (m);

chab air bubble chord length (m) (defined in App. K);

D 1- internal pipe diameter (m);
2- orifice diameter (m);

DH hydraulic diameter (m): DH = 4*AW/PW;

Dm molecular diffusivity (m2/s) of gas (see App. A);

Dp penetration depth (m) of air bubbles (measured vertically below the free-surface);

Dr turbulent diffusivity (m2/s) in the radial direction;

Ds sediment diffusion coefficient (m2/s);

Dt turbulent diffusivity (m2/s) of air bubbles in air-water flow;

Dy turbulent diffusivity (m2/s) in the y-direction;

Dl integration constant of the logarithmic velocity profile in turbulent boundary layers along a smooth plate (see App. F);

D2 integration constant of the logarithmic velocity profile in turbulent boundary layers along rough wall (see App. F);

Do ‘diffusivity’ term (m2/s) related to the longitudinal velocity gradient (see App. I);

D′ dimensionless turbulent diffusivity : D′ = Dt/((ur)Hyd*cosα*Y90);

D′′ dimensionless turbulent diffusivity defined as D′′ = (Dt*x)/(Vo*Y902) for a plane shear layer and D′′ = (Dt*x)/(Vo*r902) for a circular jet;

D* dimensionless turbulent diffusivity : D* = Dt/(V**Y90) for self-aerated flow and D* = Dt/(V**Y90) for non-aerated flow;

D# dimensionless turbulent diffusivity : D# = Dt/(Vo*yo) for two-dimensional shear flow and D# = Dt/(Vo*ro) for circular jet (see App. E);

d 1- characteristic flow thickness (m) measured normal to the flow direction;
2- flow depth (m) measured perpendicular to the channel bottom;
3- clear water flow depth defined as : =∫0Y901‐C*dy ;

dDS downstream flow depth (m) or tailwater depth (m);

dI flow depth (m) at the inception point of air entrainment in open channel (i.e. at point of apparition of ‘white’ waters);

dT transition depth (m) as deflned by STRAUB and ANDERSON (1958) (see App. G);

dab air bubble size (m);

abmin minimum air bubble size (m) detected by a probe;

(dab)max 1- maximum air bubble size (m) in turbulent shear layer;
2- maximum air bubble size (m) in self-aerated open channel flow (Chap. 13);

(dab)mean mean air bubble size (m) in turbulent shear layer;

(dab)o initial air bubble size (m);

db1 flow depth (m) at intersection of free-surface with outer edge of developing boundary layer;

dc critical flow depth (m): for a rectangular channel: c=qW2/g3;

dimpact jet thickness at nappe impact (fig. 17-5);

do 1- intake flow thickness (m);
2- nozzle diameter (m);
3- initial flow thickness (m) of free-shear layer;

dS characteristic sediment size (m);

dvc flow depth (m) at vena contracta (e.g fig. 7-2);

dl 1- upstream flow thickness (m);
2- upstream flow depth (m) (e.g. of a hydraulic jump);
3- jet thickness (m) at plunge point
4- flow thickness (m) of free-shear layer at nozzle edge;

d2 conjugate flow depth (m) of a hydraulic jump;

d50 mean sediment size (m);

d* clear water flow depth (m) at the start of the gradually-varied flow region (Chap. 10);

d′ dimensionless flow depth : d′ = d/d*;

E aeration efficiency defined in terms of dissolved gas content as : E = (CDS - CUS)/(Csat - CUS);

Eb bulk modulus of elasticity (Pa): Eb = ρ*∂P/∂ρ ;

Ec kinetic energy correction coefficient (also called Coriolis coefficient);

Eco compressibility (1/Pa): co=1ρ*∂ρ∂P;

F frequency (Hz) of oscillation of thin free-falling nappe;

Fb buoyancy force (N);

F* Froude number defined in terms of the roughness height: *=qW/g*sinα*kS3;

Fr Froude number; for a rectangular channel, it is defined as : r=qW/g*d3;

Fre Froude number at onset of air entrainment: re=Ve/g*d1;

Frimpact Froude number at nappe impact: r=qW/g*dimpact3 (see App. J);

Frvc Froude number at vena contracta;

Fro initial Froude number; for a rectangular channel: ro=qW/g*do3;

Fr1 upstream Froude number ; for a rectangular channel: r1=qW/g*d13;

Fr* Froude number defined as : r*=qW/g*d*3;

f 1- Darcy friction factor;
2- friction...

Erscheint lt. Verlag 11.10.1996
Sprache englisch
Themenwelt Sachbuch/Ratgeber
Naturwissenschaften Chemie
Naturwissenschaften Physik / Astronomie Strömungsmechanik
Technik Bauwesen
Technik Elektrotechnik / Energietechnik
Technik Maschinenbau
Technik Umwelttechnik / Biotechnologie
ISBN-10 0-08-052689-6 / 0080526896
ISBN-13 978-0-08-052689-8 / 9780080526898
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