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Transformation Mapping of Bubbles’2-D Circular Shape to
an Elliptical Shape Under Influence of a Magnetic Field in
Pool Boiling in Microgravity Conditions.
by
Thilanka Munasinghe
West Virginia University,
Morgantown, USA
thilanka.munasinghe@mail.wvu.edu.
5th MIT Fluid & CFD - June 19th 2009 1
The “Key” Terms :
• Pool Boiling
• Microgravity
• Bubble characteristics
•
5th MIT Fluid & CFD - June 19th 2009 2
What is Pool Boiling ?
How can we do pool boiling ?
Pool Boling is a method of boiling and generating bubbles in a
liquid that can boil in a container with a heat resource.
There are several ways that can do the pool boiling and one of
the common ways is boiling in a cylindrical tank as we used in
our experiment.
5th MIT Fluid & CFD - June 19th 2009 3
What is “Microgravity” ?
micro level (10-6) = μ = 0.000001
g= 9.81 m/s2 ( Earth’s gravity level)
μ g= [0.000001] X [ 9.81 ]
= 0.00000981 m/s2
5th MIT Fluid & CFD - June 19th 2009 4
Pool Boiling in two identical tanks with a
paramagnetic liquid
Paramagnetic liquid – MnCl2 (aq) + H2O
5th MIT Fluid & CFD - June 19th 2009 5
Why We need a Paramagnetic Liquid?
In order to avoid the floating of the liquid inside the tank
due to lack of gravity, paramagnetic liquid will be used
to attach the liquid to the bottom surface of the tank by
using a permanent magnet.
5th MIT Fluid & CFD - June 19th 2009 6
Bubble Behavior
• Bubble’s travel path inside the tank.
• Size of the bubble ( vertical and horizontal radius).
• Bubble’s shape deformation comparatively to the
original shape.
5th MIT Fluid & CFD - June 19th 2009 7
How to create a “Microgravity”
conditions artificially ?
Parabolic path of an aircraft can create
“Microgravity” conditions within a short period of
time such as 20-30 seconds period in a one
parabola.
5th MIT Fluid & CFD - June 19th 2009 8
Parabolic path of the aircraft that can create
microgravity condition5th MIT Fluid & CFD - June 19th 2009 9
5th MIT Fluid & CFD - June 19th 2009 10
Experiment apparatus before the flight
5th MIT Fluid & CFD - June 19th 2009 11
Closer look of the experiment set up
5th MIT Fluid & CFD - June 19th 2009 12
5th MIT Fluid & CFD - June 19th 2009 13
Boiling behavior during the
microgravity period
Boiling in Earth’s
5th MIT Fluid & CFD - June 19th 2009 14
5th MIT Fluid & CFD - June 19th 2009 15
5th MIT Fluid & CFD - June 19th 2009 16
5th MIT Fluid & CFD - June 19th 2009 17
5th MIT Fluid & CFD - June 19th 2009 18
5th MIT Fluid & CFD - June 19th 2009 19
5th MIT Fluid & CFD - June 19th 2009 20
5th MIT Fluid & CFD - June 19th 2009 21
5th MIT Fluid & CFD - June 19th 2009 22
5th MIT Fluid & CFD - June 19th 2009 23
5th MIT Fluid & CFD - June 19th 2009 24
5th MIT Fluid & CFD - June 19th 2009 25
5th MIT Fluid & CFD - June 19th 2009 26
5th MIT Fluid & CFD - June 19th 2009 27
5th MIT Fluid & CFD - June 19th 2009 28
Bubble’s coordinates on the perimeter
Three consecutive bubble frames
5th MIT Fluid & CFD - June 19th 2009 29
Colour Images has converted to gray scale images and bubble location has determined.
(1) Colour image and Gray scale image
(2) Location of the bubble on gray scale image with respect to the colour image
(1) (2)
5th MIT Fluid & CFD - June 19th 2009 30
0 0.02 0.04 0.06 0.08 0.1
0
500
1000
1500
2000
2500
3000
3500
Axial Distance Vs Magnetic Feild Strength
Axial Distance (m)
MagneticFeildStrength(Gauss)
5th MIT Fluid & CFD - June 19th 2009 31
40 45 50 55 60 65
0
5
10
15
20
25
30
35
40
45
50
Bubble Possition Vs Frame Number
Frame Number
X-CoordinateoftheBubblePossition(pixels)
5th MIT Fluid & CFD - June 19th 2009 32
0 10 20 30 40 50
20
40
60
80
100
120
140
160
180
200
220
Vertical Possition of the Bubble Vs Frame Number
Frame Number
Y-CoordinateoftheBubblePossition(pixels)
5th MIT Fluid & CFD - June 19th 2009 33
0 5 10 15 20 25 30 35 40 45 50
6
8
10
12
14
16
18
20
22
Radius Vs Frame Number
Frame Number
BubbleRadius(pixels)
Vertical Radius
Horizontal Radius
5th MIT Fluid & CFD - June 19th 2009 34
0 5 10 15 20 25 30 35 40 45 50
0
200
400
600
800
1000
1200
1400
Frame Number
BubbleArea(pixelsquard)
5th MIT Fluid & CFD - June 19th 2009 35
Possible practical applications of Pool
Boiling in microgravity
• Pool boiling in Microgravity conditions can use as a
“Cooling Process” for out of Earth conditions specially inside
the ISS (International Space Station)
• Space applications that are related to liquids and bubbles
that related to many fields such as Space medicine, Space
Agriculture, Heat transfer ..etc
5th MIT Fluid & CFD - June 19th 2009 36
Conclusion:
• In microgravity conditions boiling process take place faster than Earth’s gravity.
• At the bottom of the tank the bubble’s vertical radius is comparatively smaller than
the horizontal radius.
•As the bubble goes along the tank, the strength of the magnetic field reduces and
eventually the vertical component of the radius gets bigger than the horizontal radius.
•While the bubble travels upwards, bubble movement demonstrates a 2-D spiral path
along the tank.
•Horizontal and vertical radius, bubble area, bubble path along the vertical axis of the
tank was graphed verses bubble frame number for the detailed characteristic study of
bubbles.
•These bubbles also were observed to be elliptical and in real visualization it is in 3-D.
5th MIT Fluid & CFD - June 19th 2009 37
A. Fujiwara, Y. Danmoto, K. Hishida, “Bubble Deformation and Surrounding Flow
Structure Measured By PIV/LIV and Shadow image Technique”, ASME_JSME 4th Joint
Fluid Engineering Conference, F E DSM200 3-4 5674, Honolulu, Hawaii, USA, July
2003.
S. Toshiyuki, M. Watanabe,T. Fukano, “Study On Single Bubble Chain in Stagnant
Water”, ASME_JSME 4th Joint Fluid Engineering Conference, F E DSM200 3-4 5381,
Honolulu, Hawaii, USA, July 2003.
M. Ashihara, A. Kitagawa, M. Ishikawa, A. Nakashinchi, Y. Murai, F Yamamoto,
“Particle Tracking Velocimetry Measurement of Bubble-Bubble Interaction”,
ASME_JSME 4th Joint Fluid Engineering Conference, F E DSM200 3-4 5208,
Honolulu, Hawaii, USA, July 2003.
T. Munasinghe, “Investigating the Bubble Behavior in Pool Boiling in Microgravity
Conditions,” WCE 2008, vol. II, pp. 1366–1371, London, UK, July 2008.
C. Maneri, P Vassallo, “Dynamic of Bubble Rising in Finite and Infinite Media”
ASME_JSME 4th Joint Fluid Engineering Conference, F E DSM200 3-4 5208,
Honolulu, Hawaii, USA, July 2003.
Reference :
5th MIT Fluid & CFD - June 19th 2009 38
Acknowledgement
Special Thanks to:
NASA -West Virginia Space Grant
Consortium at WVU.
West Virginia University, College of
Engineering and Mineral Recourse.
Mechanical and Aerospace Engineering
Department of WVU.
Dr. John Kuhlman , Dr. Donald Gray,
Dr. Majid Jaraiedi , Dr. Arun Ross and
Microgravity Research Team.
Zero Gravity Cooperation.
5th MIT Fluid & CFD - June 19th 2009 39
5th MIT Fluid & CFD - June 19th 2009 40

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Pool Boiling Presentation at MIT 2009

  • 1. Transformation Mapping of Bubbles’2-D Circular Shape to an Elliptical Shape Under Influence of a Magnetic Field in Pool Boiling in Microgravity Conditions. by Thilanka Munasinghe West Virginia University, Morgantown, USA thilanka.munasinghe@mail.wvu.edu. 5th MIT Fluid & CFD - June 19th 2009 1
  • 2. The “Key” Terms : • Pool Boiling • Microgravity • Bubble characteristics • 5th MIT Fluid & CFD - June 19th 2009 2
  • 3. What is Pool Boiling ? How can we do pool boiling ? Pool Boling is a method of boiling and generating bubbles in a liquid that can boil in a container with a heat resource. There are several ways that can do the pool boiling and one of the common ways is boiling in a cylindrical tank as we used in our experiment. 5th MIT Fluid & CFD - June 19th 2009 3
  • 4. What is “Microgravity” ? micro level (10-6) = μ = 0.000001 g= 9.81 m/s2 ( Earth’s gravity level) μ g= [0.000001] X [ 9.81 ] = 0.00000981 m/s2 5th MIT Fluid & CFD - June 19th 2009 4
  • 5. Pool Boiling in two identical tanks with a paramagnetic liquid Paramagnetic liquid – MnCl2 (aq) + H2O 5th MIT Fluid & CFD - June 19th 2009 5
  • 6. Why We need a Paramagnetic Liquid? In order to avoid the floating of the liquid inside the tank due to lack of gravity, paramagnetic liquid will be used to attach the liquid to the bottom surface of the tank by using a permanent magnet. 5th MIT Fluid & CFD - June 19th 2009 6
  • 7. Bubble Behavior • Bubble’s travel path inside the tank. • Size of the bubble ( vertical and horizontal radius). • Bubble’s shape deformation comparatively to the original shape. 5th MIT Fluid & CFD - June 19th 2009 7
  • 8. How to create a “Microgravity” conditions artificially ? Parabolic path of an aircraft can create “Microgravity” conditions within a short period of time such as 20-30 seconds period in a one parabola. 5th MIT Fluid & CFD - June 19th 2009 8
  • 9. Parabolic path of the aircraft that can create microgravity condition5th MIT Fluid & CFD - June 19th 2009 9
  • 10. 5th MIT Fluid & CFD - June 19th 2009 10
  • 11. Experiment apparatus before the flight 5th MIT Fluid & CFD - June 19th 2009 11
  • 12. Closer look of the experiment set up 5th MIT Fluid & CFD - June 19th 2009 12
  • 13. 5th MIT Fluid & CFD - June 19th 2009 13
  • 14. Boiling behavior during the microgravity period Boiling in Earth’s 5th MIT Fluid & CFD - June 19th 2009 14
  • 15. 5th MIT Fluid & CFD - June 19th 2009 15
  • 16. 5th MIT Fluid & CFD - June 19th 2009 16
  • 17. 5th MIT Fluid & CFD - June 19th 2009 17
  • 18. 5th MIT Fluid & CFD - June 19th 2009 18
  • 19. 5th MIT Fluid & CFD - June 19th 2009 19
  • 20. 5th MIT Fluid & CFD - June 19th 2009 20
  • 21. 5th MIT Fluid & CFD - June 19th 2009 21
  • 22. 5th MIT Fluid & CFD - June 19th 2009 22
  • 23. 5th MIT Fluid & CFD - June 19th 2009 23
  • 24. 5th MIT Fluid & CFD - June 19th 2009 24
  • 25. 5th MIT Fluid & CFD - June 19th 2009 25
  • 26. 5th MIT Fluid & CFD - June 19th 2009 26
  • 27. 5th MIT Fluid & CFD - June 19th 2009 27
  • 28. 5th MIT Fluid & CFD - June 19th 2009 28
  • 29. Bubble’s coordinates on the perimeter Three consecutive bubble frames 5th MIT Fluid & CFD - June 19th 2009 29
  • 30. Colour Images has converted to gray scale images and bubble location has determined. (1) Colour image and Gray scale image (2) Location of the bubble on gray scale image with respect to the colour image (1) (2) 5th MIT Fluid & CFD - June 19th 2009 30
  • 31. 0 0.02 0.04 0.06 0.08 0.1 0 500 1000 1500 2000 2500 3000 3500 Axial Distance Vs Magnetic Feild Strength Axial Distance (m) MagneticFeildStrength(Gauss) 5th MIT Fluid & CFD - June 19th 2009 31
  • 32. 40 45 50 55 60 65 0 5 10 15 20 25 30 35 40 45 50 Bubble Possition Vs Frame Number Frame Number X-CoordinateoftheBubblePossition(pixels) 5th MIT Fluid & CFD - June 19th 2009 32
  • 33. 0 10 20 30 40 50 20 40 60 80 100 120 140 160 180 200 220 Vertical Possition of the Bubble Vs Frame Number Frame Number Y-CoordinateoftheBubblePossition(pixels) 5th MIT Fluid & CFD - June 19th 2009 33
  • 34. 0 5 10 15 20 25 30 35 40 45 50 6 8 10 12 14 16 18 20 22 Radius Vs Frame Number Frame Number BubbleRadius(pixels) Vertical Radius Horizontal Radius 5th MIT Fluid & CFD - June 19th 2009 34
  • 35. 0 5 10 15 20 25 30 35 40 45 50 0 200 400 600 800 1000 1200 1400 Frame Number BubbleArea(pixelsquard) 5th MIT Fluid & CFD - June 19th 2009 35
  • 36. Possible practical applications of Pool Boiling in microgravity • Pool boiling in Microgravity conditions can use as a “Cooling Process” for out of Earth conditions specially inside the ISS (International Space Station) • Space applications that are related to liquids and bubbles that related to many fields such as Space medicine, Space Agriculture, Heat transfer ..etc 5th MIT Fluid & CFD - June 19th 2009 36
  • 37. Conclusion: • In microgravity conditions boiling process take place faster than Earth’s gravity. • At the bottom of the tank the bubble’s vertical radius is comparatively smaller than the horizontal radius. •As the bubble goes along the tank, the strength of the magnetic field reduces and eventually the vertical component of the radius gets bigger than the horizontal radius. •While the bubble travels upwards, bubble movement demonstrates a 2-D spiral path along the tank. •Horizontal and vertical radius, bubble area, bubble path along the vertical axis of the tank was graphed verses bubble frame number for the detailed characteristic study of bubbles. •These bubbles also were observed to be elliptical and in real visualization it is in 3-D. 5th MIT Fluid & CFD - June 19th 2009 37
  • 38. A. Fujiwara, Y. Danmoto, K. Hishida, “Bubble Deformation and Surrounding Flow Structure Measured By PIV/LIV and Shadow image Technique”, ASME_JSME 4th Joint Fluid Engineering Conference, F E DSM200 3-4 5674, Honolulu, Hawaii, USA, July 2003. S. Toshiyuki, M. Watanabe,T. Fukano, “Study On Single Bubble Chain in Stagnant Water”, ASME_JSME 4th Joint Fluid Engineering Conference, F E DSM200 3-4 5381, Honolulu, Hawaii, USA, July 2003. M. Ashihara, A. Kitagawa, M. Ishikawa, A. Nakashinchi, Y. Murai, F Yamamoto, “Particle Tracking Velocimetry Measurement of Bubble-Bubble Interaction”, ASME_JSME 4th Joint Fluid Engineering Conference, F E DSM200 3-4 5208, Honolulu, Hawaii, USA, July 2003. T. Munasinghe, “Investigating the Bubble Behavior in Pool Boiling in Microgravity Conditions,” WCE 2008, vol. II, pp. 1366–1371, London, UK, July 2008. C. Maneri, P Vassallo, “Dynamic of Bubble Rising in Finite and Infinite Media” ASME_JSME 4th Joint Fluid Engineering Conference, F E DSM200 3-4 5208, Honolulu, Hawaii, USA, July 2003. Reference : 5th MIT Fluid & CFD - June 19th 2009 38
  • 39. Acknowledgement Special Thanks to: NASA -West Virginia Space Grant Consortium at WVU. West Virginia University, College of Engineering and Mineral Recourse. Mechanical and Aerospace Engineering Department of WVU. Dr. John Kuhlman , Dr. Donald Gray, Dr. Majid Jaraiedi , Dr. Arun Ross and Microgravity Research Team. Zero Gravity Cooperation. 5th MIT Fluid & CFD - June 19th 2009 39
  • 40. 5th MIT Fluid & CFD - June 19th 2009 40