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VOID FRACTION AND BUBBLE
DISTRIBUTION MEASUREMENT
IN BUBBLE COLUMN REACTOR
BY PRANESH KUMAR SAHA
BME-IV 001511201113
UNDER GUIDANCE OF:
SOURAV SARKAR
BUBBLE COLUMN REACTOR
•A two phase reactor operating with liquid in bulk
and gas bubbles
•Used widely in fields like biochemical,
metallurgical and petrochemical
•Design parameters: Specific gas-liquid interfacial
area, Sauter mean bubble diameter, heat transfer
coefficient, physio-chemical properties and gas
hold-up
•Gas bubble sizes and their holdups, among other
parameters, is required for proper operation,
modeling and optimization of multiphase reactors
WHY A NEW ALGORITHM
& EXPERIMENTAL SETUP
•Past experiments have used high speed
camera which are expensive
•Expensive setups are not portable and
reproducible easily
•Main motive was to develop a fast and
computationally inxpensive algorithm that can
work on images from ordinary digital camera
•Setup consists 2 rotometers, one glass tube ,an
open air circuit and closed water circuit
•Only the air circuit is used in the experiment
•LED Light and paper diffuser
FLOW REGIMES
ALGORITHM
Input
Conversion to
grey
Image
segmentation
Morphological
Opening
Image
Thinning
Branch
Removal &
Marking
End Point
Extraction
Image
Compression
Convexity
Calculation
Distance
Based
Grouping
Fitting and
Output
Main steps in the algorithm are:
1. Resonace based segmentation with
adaptive threshold
2. Thinning By Zhang Suen algorithm
3. Unwanted Branch Removal
4. Marking of separate branches
5. Convexity based grouping and distance
based selection
6. Curve fitting
Images
RESULTS &
DISCUSSION
• Starting from bottom clockwise
the volume flow-rates are .256
and .446 lit/min
• Equally distributed in low
volume flow rate of .25
• As volume flow rate increases
number of smaller bubbles
increase
• The maximum bubble diameter
also increases
• The flow is
RESULTS &
DISCUSSION(cont.)
The flow rates
are .566, .633, .737 and
1.030 l/mim
The first three are tranisent
and 1.03 has reached
heterogenous flow
Results & Discussion(cont.)
• The top graph shows flow rate of 1.4 while the bottom one
shows 3.11 l/min
• It is very evident from the images that the flow has entered
churn-turbulen or heterogenous flow regime
RESULTS &
DISCUSSION(cont.)
• The number of bubbles first increase to a maxima and then start
decreasing
• Void fraction shows a general increasing trend with a local
minima at 1.4 l/min and also number of bubbles decrease at
1.4l/min
• This is very important as it marks the onset of churn turbulent
zone.
• The values of void fraction are not accurate as only bubble rich
zones were analysed and total cylinder volume was not
considered
CONCLUSION
• The project aimed at developing a new algorithm for bubble
detection and quantification from low quality images(as compared to
others).
• The results conform suitably with existing literature showing that the
algorithm works accurately with room for improvements.
• A distinct trasient flow region can be seen by the presence of few
large sized bubbles formed by coallesence of smaller ones

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Advanced project on study of system hahumna

  • 1. VOID FRACTION AND BUBBLE DISTRIBUTION MEASUREMENT IN BUBBLE COLUMN REACTOR BY PRANESH KUMAR SAHA BME-IV 001511201113 UNDER GUIDANCE OF: SOURAV SARKAR
  • 2. BUBBLE COLUMN REACTOR •A two phase reactor operating with liquid in bulk and gas bubbles •Used widely in fields like biochemical, metallurgical and petrochemical •Design parameters: Specific gas-liquid interfacial area, Sauter mean bubble diameter, heat transfer coefficient, physio-chemical properties and gas hold-up •Gas bubble sizes and their holdups, among other parameters, is required for proper operation, modeling and optimization of multiphase reactors
  • 3. WHY A NEW ALGORITHM & EXPERIMENTAL SETUP •Past experiments have used high speed camera which are expensive •Expensive setups are not portable and reproducible easily •Main motive was to develop a fast and computationally inxpensive algorithm that can work on images from ordinary digital camera •Setup consists 2 rotometers, one glass tube ,an open air circuit and closed water circuit •Only the air circuit is used in the experiment •LED Light and paper diffuser
  • 5. ALGORITHM Input Conversion to grey Image segmentation Morphological Opening Image Thinning Branch Removal & Marking End Point Extraction Image Compression Convexity Calculation Distance Based Grouping Fitting and Output Main steps in the algorithm are: 1. Resonace based segmentation with adaptive threshold 2. Thinning By Zhang Suen algorithm 3. Unwanted Branch Removal 4. Marking of separate branches 5. Convexity based grouping and distance based selection 6. Curve fitting
  • 7. RESULTS & DISCUSSION • Starting from bottom clockwise the volume flow-rates are .256 and .446 lit/min • Equally distributed in low volume flow rate of .25 • As volume flow rate increases number of smaller bubbles increase • The maximum bubble diameter also increases • The flow is
  • 8. RESULTS & DISCUSSION(cont.) The flow rates are .566, .633, .737 and 1.030 l/mim The first three are tranisent and 1.03 has reached heterogenous flow
  • 9. Results & Discussion(cont.) • The top graph shows flow rate of 1.4 while the bottom one shows 3.11 l/min • It is very evident from the images that the flow has entered churn-turbulen or heterogenous flow regime
  • 10. RESULTS & DISCUSSION(cont.) • The number of bubbles first increase to a maxima and then start decreasing • Void fraction shows a general increasing trend with a local minima at 1.4 l/min and also number of bubbles decrease at 1.4l/min • This is very important as it marks the onset of churn turbulent zone. • The values of void fraction are not accurate as only bubble rich zones were analysed and total cylinder volume was not considered
  • 11. CONCLUSION • The project aimed at developing a new algorithm for bubble detection and quantification from low quality images(as compared to others). • The results conform suitably with existing literature showing that the algorithm works accurately with room for improvements. • A distinct trasient flow region can be seen by the presence of few large sized bubbles formed by coallesence of smaller ones