SHAPE AND RISING VELOCITY OF BUBBLES VSB-Technical University of Ostrava Faculty of Metallurgy and...
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Transcript of SHAPE AND RISING VELOCITY OF BUBBLES VSB-Technical University of Ostrava Faculty of Metallurgy and...
SHAPE AND RISING SHAPE AND RISING VELOCITY OF BUBBLESVELOCITY OF BUBBLES
VSB-Technical University of OstravaVSB-Technical University of Ostrava
Faculty of Metallurgy and Material EngineeringFaculty of Metallurgy and Material EngineeringDepartment of Chemistry, Department of Chemistry, 70833 Ostrava Poruba, CR 70833 Ostrava Poruba, CR Phone: 420 596 994 328, Fax: 420 596 918 647, e-mail: Phone: 420 596 994 328, Fax: 420 596 918 647, e-mail: [email protected]@vsb.cz
36th Conference of Slovak Society of Chemical EngineeringMay 25 - 29, 2009 Tatranské Matliare
Kamil Wichterle, Kateřina Smutná, Marek VečeřKamil Wichterle, Kateřina Smutná, Marek Večeř
Everyting is known about bubbles Everyting is known about bubbles
Clift, R., Grace, J.R. and Weber, M.E., 1978: Clift, R., Grace, J.R. and Weber, M.E., 1978: Bubbles, Drops, and ParticlesBubbles, Drops, and Particles. Academic Press, . Academic Press, New York.New York.
?
Classes of bubblesClasses of bubbles
SmallSmall bubbles in bubbles in high-viscosityhigh-viscosity liquids liquids
SmallSmall bubbles in bubbles in low-viscositylow-viscosity liquids liquids
MediumMedium bubbles in bubbles in high-viscosityhigh-viscosity liquids liquids
MediumMedium bubbles in bubbles in purepure low-viscositylow-viscosity liquidsliquids
MediumMedium bubbles in bubbles in contaminedcontamined low-low-viscosityviscosity liquids liquids
LargeLarge bubbles bubbles
SIZE OF RISING BUBBLES
increasing volume
gd
Eo B
2
LIQUID VISCOSITY
BB Ud
Re
Low– and medium-viscosity …. Re > 50
PURE OR CONTAMINED LIQUID
NO QUANTITATIVE PARAMETER !!!
•Pure liquid (surface-active components carefully removed)
•Mobil surface
•Lower drag resistance
•Higher rising velocity
•Contamined liquid•Immobile surface
•Drag like for solid bodies
•Lower rising velocity
Focus of our interestFocus of our interest
SmallSmall bubbles bubbles
MediumMedium bubbles in bubbles in purepure low-viscositylow-viscosity liquidsliquids
MediumMedium bubbles in bubbles in contamined contamined low-low-viscosityviscosity liquids liquids
LargeLarge bubbles bubbles
EASY EXPERIMENTS, SIMPLE THEORY Stokes (or Hadamard-Rybczinski) -law
COMPLICATED EXPERIMENTS
PULSATING BUBBLE SHAPE AND VELOCITY, FREQUENT BREAKUP
ELLIPSOIDAL BUBBLES, THE MOST COMMON IN BUBBLE COLUMNS
LOWER DRAG (hypothetical)
Why not ??
Hydrostatics
Surface tension
BUBBLE SHAPE
SYMMETRIC OBLATE BUBBLE
Our laboratories
DETERMINATION OF THE DETERMINATION OF THE SHAPE OF BUBBLESSHAPE OF BUBBLES
MIRROR FRONT
y x
zax
ay
LIQ
UID
FLO
W
Bubble levitating
in dowstream flow
IDEAL OBLATE ELLIPSOIDIDEAL OBLATE ELLIPSOIDsemiaxes semiaxes a, ba, b
-1,000
-0,800
-0,600
-0,400
-0,200
0,000
0,200
0,400
0,600
0,800
1,000
-1,000 -0,500 0,000 0,500 1,000
-1,000
-0,800
-0,600
-0,400
-0,200
0,000
0,200
0,400
0,600
0,800
1,000
-1,000 -0,800 -0,600 -0,400 -0,200 0,000 0,200 0,400 0,600 0,800 1,000
Standard procedure how to approximate the bubble:
•Determination of the projected bubble area
•Determination of perimeter (usually overestimated)
Calculated shape of a circle
1
1,5
2
2,5
3
3,5
4
0,1 1 10 100
Error in perimeter determination, %
Ap
pa
ren
t v
alu
e a
/b
Image analysis
IDEAL OBLATE ELLIPSOIDIDEAL OBLATE ELLIPSOIDsemiaxes semiaxes a, ba, b
-1,000
-0,800
-0,600
-0,400
-0,200
0,000
0,200
0,400
0,600
0,800
1,000
-1,000 -0,500 0,000 0,500 1,000
Improved procedure:
Determination of the object width, height and inclination•In front view
•In side view
Untreated dataUntreated data
0
2
4
6
0 2 4 6 8 10 12 14
a [mm]
b [
mm
]
waterwater-CaCl2glycerolbutanol
Reynolds number ?Reynolds number ?
1,01,11,21,31,41,51,61,71,81,92,0
1 10 100 1000 10000
Re
(2a/
d)2
w aterw ater-CaCl2glycerolbutanol
Weber number ?Weber number ?
1,01,11,21,31,41,51,61,71,81,92,0
1 10 100
We
(2a/
d)2
w aterw ater-CaCl2glycerolbutanol
LBB ud
eW2
Eötvös numberEötvös number
1,0
1,11,2
1,3
1,41,5
1,6
1,7
1,81,9
2,0
0,1 1 10 100
Eo
(2a/
d)2
w aterw ater-CaCl2glycerolbutanolstatic bubble
gd
Eo B
2
Static bubble profileStatic bubble profile(under a wetted plate)(under a wetted plate)
-3
-2
-1
0
0 1 2 3 4 5 6 7x/L
y/L
gL
„Laplace length!“
Normalized semiaxes of rising bubblesNormalized semiaxes of rising bubbles
Theoretical prediction for static bubblesTheoretical prediction for static bubbles
20for095.012 75.0
2
EoEod
a
0
1
2
3
0 1 2 3 4 5 62a/L
2b/L water
water-CaCl2glycerolbutanolWellek (drops)static bubble
RISING VELOCITYRISING VELOCITY
Rising velocity records for 7 bubbles of volume150 mm3 in water
0.21
0.22
0.23
0.24
0.25
0.26
0 200 400 600 800 1000 1200 1400
frame number (125 frame/s)
uB (m
/s)
Time = 10 s , (corresponding path 2,3 m)
RISING VELOCITYRISING VELOCITY for medium contaminated bubblesfor medium contaminated bubbles
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 0.009 0.01
d , m
u m/s
H2O
CaCl2 1%
Glycerol 70%
Glycerol 73%
Butanol
Effects of
•Viscosity
•Surface tension
•Electrolyte
Our data compared with that of CliftOur data compared with that of Clift
H2O+CaCl2H2O
Our data compared with that of TomiyamaOur data compared with that of Tomiyama
H2O+CaCl2
H2O
RISING VELOCITYRISING VELOCITY dimensional analysisdimensional analysis
,,,,, gdfuRising velocity
•Bubble equivalent diameter
•Gravity acceleration
•Liquid density
•Density difference
•Liquid viscosity
•Surface tension
RISING VELOCITYRISING VELOCITY effect of surface tensioneffect of surface tension
41
g
W
21
41
Eo
MoeR
W
uU
2
1
21
EoL
d
g
dD
„Laplace velocity“
Dimensionless bubble diameter
Dimensionless bubble velocity
0.5
1.0
1.5
2.0
2.5
3.0
0 2 4 6 8 10 12 14 16 18 20
d/L
u/W
H2O
CaCl2 1%
Glycerol 70%
Glycerol 73%
Butanol
Viscosity cannot be neglected !!
Morton number
3
4gMo
RISING VELOCITYRISING VELOCITY classical variablesclassical variables
22 3
4
3
4
u
dg
u
dgCD
Drag coefficient
0.1
1
10
10 100 1000 10000Re
D
H2O
CaCl2 1%
Glycerol 70%
Glycerol 73%
Butanol
contaminated liquid
pure liquid
Not very successful !!
RISING VELOCITYRISING VELOCITY effect of viscosityeffect of viscosity
Dimensionless bubble diameter
Dimensionless bubble velocity
3
13
2
31
32
3
4DCeR
g
dD
22 3
4
3
4
u
dg
u
dgCD
Drag coefficient
31
31
3
4
DC
eR
g
uU
0
2
4
6
8
10
12
0 50 100 150 200 250D
U
Eo=1-2
Eo=2-3
Eo=3-4
Eo=4-5
Eo=5-7
Eo=7-10
Eo=10-20
There is still an effect of surface tension!!
RISING BUBBLERISING BUBBLE horizontal velocity
rising velocity
amplitude
Oscillatory movement of a Oscillatory movement of a bubble bubble
Bubble front area isBubble front area isSS = = aa22
New definition of the New definition of the drag coefficientdrag coefficient
2
2
2
23
4
2
a
d
u
gd
a
dCC DA
New dimensionless variablesNew dimensionless variables 3/2
2
a
dUU a
3/2
2
a
dDD a
0
2
4
6
8
10
12
14
0 50 100 150 200 250
Eo=1-2
Eo=2-3
Eo=3-5
Eo=5-10
Eo=10-20
D a
U a
OK !!!
RESULTING FORMULASRESULTING FORMULASCorrelation of the bubble shapeCorrelation of the bubble shape
Correlation of the bubble velocityCorrelation of the bubble velocity
20for095.012 75.0
2
EoEod
a
This correlation fits well the data for medium size bubbles in contaminated low- and medium- viscosity liquids. In carefully prepared pure liquids, the rising velocity of can be somewhat higher.
30,201for
095.01365.0 75.0143.0
ReEo
EoeRCD
Thank you for your attentionThank you for your attention
Acknowledgments We gratefully acknowledge financial support by the grant No.104/07/1110 from the Grant Agency of the Czech
Republic.