Title: Interacting Bubbles
1 Interacting Bubbles
2Outline
- I. Interaction of Oscillating Bubbles
- Introduction Relevance
- Experimental apparatus and results
- Mathematical model and computer simulations
3I. Interaction of Oscillating Bubbles
- Acoustic forcing pA(t)
- Bubble pulsation
- Secondary waves
- Interaction forces
4Introduction
- Degassing of the melt in microgravity
- acoustic cavitation
- ultrasonics degassing and medical ultrasonic
diagnostics - bubble sonoluminescence
5RELEVANCE to Microgravity
- De-gassing liquids and melts (NASA Microgravity
Crystal growth techniques)
6RELEVANCE - others
- Prevention of erosion due to cavitation
7Experimental set up
8ACOUSTIC LEVITATION
9Acoustic 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
10PULSATION MODEL
- Harmonic response
- Frequency ratio
- Resonance frequency
11BUBBLE 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
12INTERACTION 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
13Harmonic 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
14Damping 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
15Attracting bubbles
166 ms 233 ms 266 ms 299 ms 333 ms 366 ms
88 ms 112 ms 120 ms 128 ms 136 ms
16Relative 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
17Outcome 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
18Investigation 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
19Investigation of coalesce lag (2)
- For bubble size ratio ? 2
- time lag ( 15 sec - 45 sec)
20Near-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
21Two 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
22Relative 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
23Relative 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
24Force 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
25Three 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
26History 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
27Other 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
28Discussion
- 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
29Summary
- 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
30BUBBLE CLOUD MODEL
- Interaction forces Fji
- Drag force Di
- Resultant Fi
- Velocity Vi
31BUBBLE CLOUD MODEL
32BUBBLE CLOUD MODEL
33EVOLUTION PATTERNS
- Coalescence
- Dispersion
- Transition to equilibrium
- Vibration
- Combined patterns
34CONCLUSIONS AND RECOMMENDATIONS
35Future work
- Multi-bubble dynamics
- Two dimensional motion of the bubbles
- Bubble behavior in various acoustic environment
36History Location of the bubbles
set t0 at r010 R0
set t0 at r020 R0
37Numerical solution for velocity and acceleration
II
III
I
II
III
I
38Secondary Bjerknes force drag force
39Velocity 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
40Error Analysis
41Boundary condition
- Parallel case for two attracting bubbles
- use image source to replace the rigid wall
- phase difference ignored (?gtgtx)
Physical condition
Image geometry
42Mathematical 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
43Model 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
44Relative 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
45Boundary effect compared between two experiments
46Error Analysis (1)
47Error Analysis (2)
48Primary 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
49Secondary 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
50Experiment methods and procedures
- Experimental apparatus and set up
- Experimental methods
- Forcing amplitude on the levitation plane
51Experimental 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
52Forcing amplitude
- Buoyancy force
- Primary Bjerknes force
- Forcing Amplitude
- Forcing Amplitude on
- the levitation plane
53Experimental 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
54Mathematical models for non-resonant pair
- Virtual mass of each bubble
- Secondary Bjerknes force
- Drag force
- Initial condition vv0 at rr0