2022
DOI: 10.1016/j.ijheatmasstransfer.2022.123234
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Investigation of film boiling at a liquid-liquid contact

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Cited by 4 publications
(1 citation statement)
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“…For atmospheric codition simulations (in a λ B × λ B domain), the vapor–liquid interface was provided following the equation y = λ 64 true( 4 + cos ( 2 π x λ ) true) where λ is Taylor’s most dangerous wavelength, and y is the thickness of the film. The equation is commensurate with the conditions used by Dixit et al For the larger domain simulations (3λ B × 3λ B ), a similar equation was adopted with the multiplication of random numbers. The bulk liquid was considered at a constant temperature T sat throughout the simulation.…”
Section: Methodsmentioning
confidence: 99%
“…For atmospheric codition simulations (in a λ B × λ B domain), the vapor–liquid interface was provided following the equation y = λ 64 true( 4 + cos ( 2 π x λ ) true) where λ is Taylor’s most dangerous wavelength, and y is the thickness of the film. The equation is commensurate with the conditions used by Dixit et al For the larger domain simulations (3λ B × 3λ B ), a similar equation was adopted with the multiplication of random numbers. The bulk liquid was considered at a constant temperature T sat throughout the simulation.…”
Section: Methodsmentioning
confidence: 99%