1988
DOI: 10.13182/fst88-a25140
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A Phenomenological Model for Prediction of Critical Heat Flux under Highly Subcooled Conditions

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Cited by 97 publications
(8 citation statements)
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“…The critical void fraction a b is empirically set at 0.82, which corresponds to oval bubbles with long to short radius ratio of 3 to 1 are packed in the bubbly layer. To adapt the model better to high subcooling region, Weisman and Ileslamlou [6] extended the Weisman-Pei model by using basic energy balance for the bubbly layer to compute the CHF. The approaches of Weisman and coworkers show good accuracy to high-pressure water data, liquid nitrogen data and Feron 113 data.…”
Section: Bubble Crowding Modelmentioning
confidence: 99%
“…The critical void fraction a b is empirically set at 0.82, which corresponds to oval bubbles with long to short radius ratio of 3 to 1 are packed in the bubbly layer. To adapt the model better to high subcooling region, Weisman and Ileslamlou [6] extended the Weisman-Pei model by using basic energy balance for the bubbly layer to compute the CHF. The approaches of Weisman and coworkers show good accuracy to high-pressure water data, liquid nitrogen data and Feron 113 data.…”
Section: Bubble Crowding Modelmentioning
confidence: 99%
“…In addition, they revised the calculation for bubble diameters and included the slip ratio in the bubble layer to improve CHF prediction at low mass flow rates. Weisman and Illeslamlou (1988), on the other hand, extended the model to high subcooling conditions based on the energy balance at the outer edge of the bubble layer in round tubes. Chang and Lee (1989) revised the calculation of the lateral mass velocity from the core to the bubble layer at low qualities in uniformly heated tubes in their CHF model.…”
Section: Introductionmentioning
confidence: 99%
“…boundary layer separation model (Tong, 1968), bubble crowding model (Joel Weisman, 1988), interfacial lift-off model (Galloway and Mudawar, 1993b), sublayer dryout model (Lee and Mudawwar, 1988), have been postulated as the trigger for CHF in subcooled and near-saturated flow boiling. All these mechanisms were based upon some physical process that blocks fresh liquid flow from reaching the heated wall.…”
Section: Introductionmentioning
confidence: 99%