000 | 02099aab a2200205 4500 | ||
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008 | 240131b19901990|||mr||| |||| 00| 0 eng d | ||
022 | _a0017-9310 | ||
100 |
_aMohamed S. El-Genk _9880286 |
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100 |
_aDasari V. Rao _9880288 |
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245 | _aBuoyancy Induced Instability of Laminar Flows in Vertical Annuli—I. Flow Visualization and Heat Transfer Experiments | ||
300 | _a2145-2159 p. | ||
520 | _aExperiments encompassing both flow visualization and heat transfer measurements (125 < Rein < 1700 and 2.5 × 105 < Grq < 5 × 107) are performed to investigate buoyancy induced instability of developing laminar upflow and downflow of water in a vertical annulus having a diameter ratio of 2.0. The inner wall of the annulus is uniformly heated and the outer wall is insulated. Incipient flow instability is detected from the video images of the dyed flow field, the simultaneous decrease in the temperature difference between the heated wall and the water bulk from its laminar value and the fluctuations in the coolant temperature. The measured values of xfr, based on the video images of the dyed flow fields, are correlated for both buoyancy assisted and opposed flows as functions of local Grashof number, Grq, and local Reynolds number, Re. The Nusselt numbers for buoyancy induced turbulent flows. occurring downstream of the location of incipient instability, are as much as three times higher than those for stable laminar flows at the same inlet Reynolds number, but at lower Grq. The heat transfer data for buoyancy induced turbulent flows are correlated as: Nu = 0.088Raq0.33Rein−0.12, for upflow Nu = 0.21Raq0.29Rein−0.12, for downflow. | ||
650 |
_aBuoyancy Induced Instability _9880587 |
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650 |
_aLaminar Flows _9880588 |
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650 |
_aVertical Annuli _9865363 |
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650 |
_aFlow Visualization _9116118 |
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773 | 0 |
_tInternational Journal of Heat and Mass Transfer _x00179310 _dNew York, U.S.A : Pergamon Subsidiary of Elsevier Science & Technology |
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856 | _uhttps://www.sciencedirect.com/science/article/pii/001793109090116C | ||
942 |
_2ddc _n0 _cART _o14993 _pMr. Muhammad Rafique Al Haj Rajab Ali (Late) |
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999 |
_c814900 _d814900 |