TY - GEN
T1 - Flow regime identification in large diameter pipe
AU - Sawant, Pravin
AU - Schelegel, Joshua
AU - Paranjape, Sidharth
AU - Ozar, Basar
AU - Hibiki, Takashi
AU - Ishii, Mamoru
N1 - Publication details (e.g. title, author(s), publication statuses and dates) are captured on an “AS IS” and “AS AVAILABLE” basis at the time of record harvesting from the data source. Suggestions for further amendments or supplementary information can be sent to [email protected].
PY - 2008
Y1 - 2008
N2 - Air-water vertical two-phase flow experiments were performed in a 0.15 m diameter and 4.4 m long test section. Superficial liquid velocity was varicd from 0.05 m to 2.0 m and superficial gas velocity was varied to obtain the area averaged void fraction range of 0.1 to 0.7. Exit pressure was close to the atmospheric pressure. In order to study the development of flow structure over the length of test section, area averaged void fraction was measured using impedance meters at four different measuring ports. Pressure drop was also measured between these ports. Since the temporal variation of void fraction signal obtained from the impedance meter and its distribution are characteristic of the flow regime, a Cumulative Probability Distribution Function (CPDF) of the void fraction signal was utilized for the identification of flow regime at each port. The CPDFs of the impedance probe void fraction signal were supplied as an input to the Kohonen Self Organized neural network or the Self Organized Map (SOM) for the identification of the patterns by employing self organized neural network technique. The three flow regimes identified by the neural network are subjectively named as bubbly flow, cap- bubbly flow and cap-turbulent flow. © 2008 by ASME.
AB - Air-water vertical two-phase flow experiments were performed in a 0.15 m diameter and 4.4 m long test section. Superficial liquid velocity was varicd from 0.05 m to 2.0 m and superficial gas velocity was varied to obtain the area averaged void fraction range of 0.1 to 0.7. Exit pressure was close to the atmospheric pressure. In order to study the development of flow structure over the length of test section, area averaged void fraction was measured using impedance meters at four different measuring ports. Pressure drop was also measured between these ports. Since the temporal variation of void fraction signal obtained from the impedance meter and its distribution are characteristic of the flow regime, a Cumulative Probability Distribution Function (CPDF) of the void fraction signal was utilized for the identification of flow regime at each port. The CPDFs of the impedance probe void fraction signal were supplied as an input to the Kohonen Self Organized neural network or the Self Organized Map (SOM) for the identification of the patterns by employing self organized neural network technique. The three flow regimes identified by the neural network are subjectively named as bubbly flow, cap- bubbly flow and cap-turbulent flow. © 2008 by ASME.
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U2 - 10.1115/ICONE16-48311
DO - 10.1115/ICONE16-48311
M3 - RGC 32 - Refereed conference paper (with host publication)
SN - 0791848159
SN - 9780791848159
VL - 3
T3 - International Conference on Nuclear Engineering, Proceedings, ICONE
SP - 341
EP - 351
BT - 2008 Proceedings of the 16th International Conference on Nuclear Engineering, ICONE16
T2 - 16th International Conference on Nuclear Engineering, ICONE16 2008
Y2 - 11 May 2008 through 15 May 2008
ER -