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This paper presents how a single rising bubble experiment in the Hallimond Tube can be predicted using computational fluid dynamics model. The study is emphasized on the effect of aspect ratio of cylinder domain to the pressure coefficient and axial velocity around the bubble. A rigid sphere with the radius of 0.00575 m using flow velocity of 0.25 m/s is considered in this study. Numerical and simulated data obtained by other researchers in the similar study were used to validate the simulation results fromcomputational fluid dynamics model. It was observed that a change in width in aspect ratio, causing significant change in the value of simulation data. The highest percentage of difference was observed at the vicinity of θ = 85.26 o which is 32.4%.
Ashraf Azmi. 2014. \u201cSensitivity of the Computational Domain Aspect Ratio for a Single Rising Bubble in a Hallimond Tube\u201d. Global Journal of Research in Engineering - C: Chemical Engineering GJRE-C Volume 14 (GJRE Volume 14 Issue C1): .
Crossref Journal DOI 10.17406/gjre
Print ISSN 0975-5861
e-ISSN 2249-4596
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Total Score: 101
Country: Malaysia
Subject: Global Journal of Research in Engineering - C: Chemical Engineering
Authors: Ashraf Azmi (PhD/Dr. count: 0)
View Count (all-time): 202
Total Views (Real + Logic): 4638
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Publish Date: 2014 06, Mon
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This paper presents how a single rising bubble experiment in the Hallimond Tube can be predicted using computational fluid dynamics model. The study is emphasized on the effect of aspect ratio of cylinder domain to the pressure coefficient and axial velocity around the bubble. A rigid sphere with the radius of 0.00575 m using flow velocity of 0.25 m/s is considered in this study. Numerical and simulated data obtained by other researchers in the similar study were used to validate the simulation results fromcomputational fluid dynamics model. It was observed that a change in width in aspect ratio, causing significant change in the value of simulation data. The highest percentage of difference was observed at the vicinity of θ = 85.26 o which is 32.4%.
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