Investigation of flow boiling heat transfer and boiling crisis on a rough surface using infrared thermometry

© 2020 Elsevier Ltd We design and build a special heater to enable infrared investigations of boiling heat transfer on surfaces featuring the typical roughness and scratch pattern of commercial-grade heat transfer surfaces (in this case a zirconium alloy typically used as fuel cladding material in n...

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Bibliographic Details
Main Authors: Su, G-Y (Author), Wang, C (Author), Zhang, L (Author), Seong, JH (Author), Kommajosyula, R (Author), Phillips, B (Author), Bucci, M (Author)
Format: Article
Language:English
Published: Elsevier BV, 2021-11-16T13:33:55Z.
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Online Access:Get fulltext
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042 |a dc 
100 1 0 |a Su, G-Y  |e author 
700 1 0 |a Wang, C  |e author 
700 1 0 |a Zhang, L  |e author 
700 1 0 |a Seong, JH  |e author 
700 1 0 |a Kommajosyula, R  |e author 
700 1 0 |a Phillips, B  |e author 
700 1 0 |a Bucci, M  |e author 
245 0 0 |a Investigation of flow boiling heat transfer and boiling crisis on a rough surface using infrared thermometry 
260 |b Elsevier BV,   |c 2021-11-16T13:33:55Z. 
856 |z Get fulltext  |u https://hdl.handle.net/1721.1/138149 
520 |a © 2020 Elsevier Ltd We design and build a special heater to enable infrared investigations of boiling heat transfer on surfaces featuring the typical roughness and scratch pattern of commercial-grade heat transfer surfaces (in this case a zirconium alloy typically used as fuel cladding material in nuclear reactors). We use high-speed infrared thermometry to investigate surface effects on the boiling process for both the rough infrared heater and a reference more conventional, nano-smooth infrared heater. Compared to the nano-smooth surface, the rough surface has larger nucleation sites, which require a lower nucleation temperature. The rough surface has a much smaller bubble departure volume. However, it has a much higher nucleation site density, and, overall, a higher heat transfer coefficient. We capture this behavior with a stochastic heat flux partitioning model. Notably, while the two surfaces have very different boiling dynamics, the boiling crisis has a common "signature". For both surfaces, the probability density functions of bubble footprint areas follow a power law with a negative exponent smaller than 3, also known as a scale-free distribution. We predict these observations and the onset of the boiling crisis using a continuum percolation model. These results corroborate the hypothesis of the boiling crisis as a percolative critical phase transition of the bubble interaction process. 
546 |a en 
655 7 |a Article 
773 |t 10.1016/J.IJHEATMASSTRANSFER.2020.120134 
773 |t International Journal of Heat and Mass Transfer