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Interacting Bubbles

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Levitation Chamber. Distilled Water ... high ratio in the large spacing caused by the pressure gradient in the levitation plane ... – PowerPoint PPT presentation

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Title: Interacting Bubbles


1

Interacting Bubbles
2
Outline
  • I. Interaction of Oscillating Bubbles
  • Introduction Relevance
  • Experimental apparatus and results
  • Mathematical model and computer simulations

3
I. Interaction of Oscillating Bubbles
  • Acoustic forcing pA(t)
  • Bubble pulsation
  • Secondary waves
  • Interaction forces

4
Introduction
  • Degassing of the melt in microgravity
  • acoustic cavitation
  • ultrasonics degassing and medical ultrasonic
    diagnostics
  • bubble sonoluminescence

5
RELEVANCE to Microgravity
  • De-gassing liquids and melts (NASA Microgravity
    Crystal growth techniques)

6
RELEVANCE - others
  • Prevention of erosion due to cavitation

7
Experimental set up
8
ACOUSTIC LEVITATION
9
Acoustic levitator
Distilled Water
  • High-speed video images of bubbles interacting
    under acoustic forcing
  • Forcing frequency f 22.3-22.5 kHz
  • Variables R01, R02, A, d0, u0

Levitation Chamber
Piezoelectric Ceramic
Iron Base
10
PULSATION MODEL
  • Harmonic response
  • Frequency ratio
  • Resonance frequency

11
BUBBLE CLASSIFICATION
  • Resonance size R0
  • Bubble types
  • A Above resonance size, R0gtR0 , qgt1
  • X Close to resonance size, R0R0 , q1
  • B Below resonance size, R0ltR0, qlt1

12
INTERACTION FORCE
  • In phase j0 (AA, BB pairs) Attraction
  • Opposite phase jp (AB pairs) Repulsion
  • Phase shift jp/2 (XB,XA pairs) Long-range
    attraction, short-range repulsion

13
Harmonic response of a single bubble under
pressure oscillation
  • External pressure
  • Linear Response of bubble shape
  • response amplitude
  • phase difference
  • PA constant pressure (usually air pressure)
  • R0 equilibrium size
  • A oscillatory pressure amplitude
  • ? radian frequency
  • ?0 bubble natural frequency
  • ? damping coefficient

14
Damping of shape oscillation
? liquid viscosity Im (? ) complex
function c sound velocity in the liquid ?
surface tension
  • Viscous component
  • Thermal component
  • Acoustic component

Adapted from Brennen
15
Attracting bubbles
166 ms 233 ms 266 ms 299 ms 333 ms 366 ms
88 ms 112 ms 120 ms 128 ms 136 ms
16
Relative velocity of two attracting bubbles
  • R10 0.4167 mm,
  • R20 0.4167 mm
  • Az 4.2 Kpa
  • f 22 kHz
  • v0 12.5 mm/s
  • at r0 20 radii

17
Outcome of attracting bubbles
  • coalesce instantly
  • (most cases for bubble with close sizes)
  • coalesce with time lag
  • (Ri/Rjgt2) 65-70
  • collect and co-exist
  • (rare and only for big bubble size ratio)

collapse
18
Investigation of coalesce lag (1)
  • For equal size bubbles
  • Az 2.7 KPa
  • f 22.5 kHz
  • R1R2? 0.5 mm
  • v011.6 mm/s at r012 radii

19
Investigation of coalesce lag (2)
  • For bubble size ratio ? 2
  • time lag ( 15 sec - 45 sec)

20
Near-resonance coupling model
  • Interaction force
  • Coupling coefficient
  • coefficients m,n
  • Condition
  • cos? O (?1?2)
  • ?2?? ?1??/2
  • Assumption
  • ?2, ?i unchanged
  • Phenomenon
  • possible oscillation with stable equilibrium
    spacing requ
  • sign of force may change during the motion

21
Two bubble oscillation
  • Bubble sizes
  • R1 0.161 mm
  • R2 0.151 mm
  • Acoustic parameter
  • Az 1.26 KPa
  • f 20.5 kHz
  • Motion patternoscillation
  • T 0.86 s
  • amplitude 3.15 mm

22
Relative velocity versus time
  • Repulsion is much violent than attraction
  • the motion of two bubbles are generally symmetric
  • highest velocity around 20 mm/s about 4-5 times
    as large as that in approach stage

23
Relative velocity versus separation
  • Model under-predict the velocity in repulsion
    stage
  • out of balance position in levitation plane
  • loss of spherical shape at small spacing
  • model simplification

24
Force field for the resonant couple
  • Equilibrium separation requ?20 radii
  • repulsion force have a sharper change in small
    spacing
  • attraction force increase from requ with the
    increase of separation then decrease very slowly

25
Three Bubble Oscillation
  • Condition
  • R1R2?0.133 mm
  • R0 0.146 mm
  • f 22.5 kHz
  • Az 1.34 Kpa
  • Model simplification
  • x-symmetry
  • bubble 0 motionless
  • interaction between bubble 1 and bubble 2 ignored
  • coupling coefficient

26
History Location of the bubbles
  • Right bubble
  • bound 3.64 - 4.8 radii
  • frequency 16.6 Hz
  • Left bubble
  • bound 3.58 - 4.6 radii
  • frequency 16.5 Hz
  • Model
  • bound 3.68-4.82 radii
  • frequency 16.2 Hz

27
Other experimental observation
A
C
  • Experiment A
  • small bubble oscillate with big one and at the
    same time has angular motion
  • Experiment B
  • five bubbles aligned with oscillation, bubble in
    the middle shift position
  • Experiment C
  • three bubbles in same levitation plane perform
    planar oscillation

B
28
Discussion
  • System of more than two bubbles may display
    collective or evolution motion
  • Two-dimensional is likely to happen with more
    than two bubble or given initial angular motion
  • Group oscillation may not restricted to the
    condition for two-bubble oscillation

29
Summary
  • Non-resonant pair
  • motion attraction for R0gtRr
  • force a/r2, sign unchanged
  • ? and ? not change
  • conservative model
  • drag force
  • outcome of two attracting bubbles
  • Resonant pair
  • motion possible oscillation
  • force a/r2-b/r3, sign of force may change
  • ?1 changed with separation r
  • two bubble oscillation
  • repulsion violent than approach
  • three bubble oscillation
  • more bubbles and 2-D motion

30
BUBBLE CLOUD MODEL
  • Interaction forces Fji
  • Drag force Di
  • Resultant Fi
  • Velocity Vi

31
BUBBLE CLOUD MODEL
  • Equations of motion

32
BUBBLE CLOUD MODEL
  • Coupling equations

33
EVOLUTION PATTERNS
  • Coalescence
  • Dispersion
  • Transition to equilibrium
  • Vibration
  • Combined patterns

34
CONCLUSIONS AND RECOMMENDATIONS
35
Future work
  • Multi-bubble dynamics
  • Two dimensional motion of the bubbles
  • Bubble behavior in various acoustic environment

36
History Location of the bubbles
set t0 at r010 R0
set t0 at r020 R0
37
Numerical solution for velocity and acceleration
II
III
I
II
III
I
38
Secondary Bjerknes force drag force
39
Velocity ratio
  • Ratio of experimental velocity to the velocity of
    model prediction
  • ratio approach 1 with the decrease of spacing
  • high ratio in the large spacing caused by the
    pressure gradient in the levitation plane

40
Error Analysis
41
Boundary condition
  • Parallel case for two attracting bubbles
  • use image source to replace the rigid wall
  • phase difference ignored (?gtgtx)

Physical condition
Image geometry
42
Mathematical model
  • The reflected force
  • Total force
  • ? is the pressure reflection coefficient
  • reflection angle
  • ? arccos (r/y)
  • ?glass2300 kg/m3
  • velocity in glass
  • c 5200 m/s
  • x is the distance between bubble and boundary

43
Model prediction of relative velocities
  • R1 R2 0.45 mm
  • Az 3 Kpa
  • f 22.5 kHz
  • x 1mm 20 mm
  • v0 0 at r0 6 mm

44
Relative velocities in experiments
  • Bubble sizes
  • R1 0.455 mm
  • R2 0.355 mm
  • forcing amplitude
  • Az 2.55Kpa
  • f 22.5 kHz
  • v0 11 mm/s at r014 R1

45
Boundary effect compared between two experiments
46
Error Analysis (1)
47
Error Analysis (2)
48
Primary Bjerknes force
  • lt gt time average
  • P(r,t) time-and-spacing-varying pressure field
  • A amplitude of the stationary wave
  • kz?/c wave number
  • k gas polytropic number
  • General form
  • Force in a stationary sound field
  • sinusoidal pressure variation

49
Secondary pressure radiation
  • Function ?
  • phase difference between two pulsation ?
  • F12(r) F21(r)
  • Secondary wave emitted by the bubble
  • Secondary Bjerknes force

Flt0, attraction Fgt0, repulsion
50
Experiment methods and procedures
  • Experimental apparatus and set up
  • Experimental methods
  • Forcing amplitude on the levitation plane

51
Experimental methods
  • Adjust the frequency and water level to make one
    full wave length of standing wave generated by
    the acoustic levitator
  • Use high-speed camera to capture the motion of
    bubbles and measure the size/location of the
    bubble frame by frame using the movable reticle
  • Balance the buoyancy force (FBFp) to obtain the
    forcing amplitude on the levitation plane
  • Check the wave with oscilloscope and hydrophone

52
Forcing amplitude
  • Buoyancy force
  • Primary Bjerknes force
  • Forcing Amplitude
  • Forcing Amplitude on
  • the levitation plane

53
Experimental study and analysis of bubble
dynamics
  • Non-resonant bubble dynamics
  • Conservative model and drag model
  • Outcome of two attracting bubbles
  • Boundary effects
  • Resonant bubble interaction
  • 2 bubble oscillation
  • 3 bubble oscillation
  • other observations

54
Mathematical models for non-resonant pair
  • Virtual mass of each bubble
  • Secondary Bjerknes force
  • Drag force
  • Initial condition vv0 at rr0
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