Numerical Analysis of Flow Noise Characteristics of Pump-jet Propeller Based on Different Turbulence Models

Author(s):  
Xiaoxu Du ◽  
Chuang Liu ◽  
Xiaolian Zhang ◽  
Keyao Fu
2015 ◽  
Author(s):  
Guilherme Loyola França de Vasconcellos ◽  
Caio Dell'Oro de Oliveira ◽  
Antônio Augusto Mesquita Diniz ◽  
Sérgio de Morais Hanriot ◽  
Cristiana Brasil Maia

2019 ◽  
Vol 2019.29 (0) ◽  
pp. J114
Author(s):  
Suguru DOSHIDA ◽  
Hayato YOSHINAGA ◽  
Gaku MINORIKAWA ◽  
Tsunebumi MIKUNI

2015 ◽  
Vol 21 (6) ◽  
pp. 223-231 ◽  
Author(s):  
Jialin Zhao ◽  
Huijuan Zhou ◽  
Fan Liu ◽  
Yonglin Yu

AIP Advances ◽  
2017 ◽  
Vol 7 (6) ◽  
pp. 065114 ◽  
Author(s):  
Sanghyeon Kim ◽  
Cheolung Cheong ◽  
Warn-Gyu Park

2020 ◽  
Vol 66 (9) ◽  
pp. 544-553
Author(s):  
Urban Močnik ◽  
Bogdan Blagojevič ◽  
Simon Muhič

A plate heat exchanger with a dimple pattern heat plate has a large number of dimples. The shape of dimples defines the characteristics of the plate heat exchanger. Although such heat exchangers have become increasingly popular due to their beneficial characteristics, knowledge of the flow characteristics in such kind of channel is poor. A good knowledge of the flow conditions inside of such channel is crucial for the successful and efficient development of new products. In this paper single-phase water flow in dimple pattern plate heat exchanger was investigated with application of computational fluid dynamics and laboratory experiments. Numerical analysis was performed with two turbulence models, Realizable - with enhanced wall treatment function and - SST. The first predicts a slightly smaller pressure drop and the second slightly larger compared to the results of laboratory measurements. Our research found that despite the relatively low velocity of the fluid, turbulent flow occurs in the channel due to its shape. We also found that there are two different flow regimes in the micro plate heat exchanger channel. The first regime is the regime that dominates the heat transfer, and the second is the regime where a recirculation zone appears behind the brazing point, which reduces the surface for heat transfer. The size of the second regime does not change significantly with the velocity of the fluid in the volume considered.


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