scholarly journals Fully developed turbulent flow in a square duct with a rough wall.

1987 ◽  
Vol 53 (492) ◽  
pp. 2370-2376 ◽  
Author(s):  
Hideomi FUJITA ◽  
Hajime YOKOSAWA ◽  
Masafumi HIROTA ◽  
Satoru NISHIGAKI
1993 ◽  
Vol 59 (561) ◽  
pp. 1510-1517 ◽  
Author(s):  
Hitoshi Sugiyama ◽  
Mitsunobu Akiyama ◽  
Masashi Matsumoto ◽  
Masaru Hirata ◽  
Nao Ninomiya

1993 ◽  
Vol 59 (561) ◽  
pp. 1502-1509 ◽  
Author(s):  
Hitoshi Sugiyama ◽  
Mitsunobu Akiyama ◽  
Masashi Matsumoto ◽  
Masaru Hirata ◽  
Nao Ninomiya

1989 ◽  
Vol 55 (510) ◽  
pp. 351-357
Author(s):  
Mitsunobu AKIYAMA ◽  
Hiroshi KAWAMURA ◽  
Toshiyuki SERIZAWA ◽  
Hitoshi SUGlYAMA ◽  
Tomoaki KUNUGI ◽  
...  

2020 ◽  
Author(s):  
Limin Wang ◽  
Tao Hu ◽  
Xing Xiang ◽  
Wei Ge

Abstract Using multi-GPU in lattice Boltzmann method (LBM), fully developed turbulent flow in a square duct at the friction Reynolds numbers (Reτ) of 300, 600, 1200 and 1800 are simulated. Through simulation of three-dimensional lid-driven cavity flow under different Reynolds number (Re), the accuracy of lattice Bhatnager-Gross-Krook (LBGK) multi-GPU program is validated. For turbulent flow in a square duct, all mean velocity, secondary flows, root mean square (rms) of pulsating velocity and Reynolds shear stress predicted by LBGK under the lower Reτ agree well with the literature results, which further verified the effectiveness of the LBGK. In addition, fully developed turbulent flow in a square duct with Reτ up to 1800 predicted by LBGK with 600 million grids provides a reference for turbulent flows under high Reτ . Numerical results show that the LBGK model with low accuracy successfully captures turbulent characteristics for flows at high Re by increasing the grid size, indicating the feasibility and practicality of multi-GPU LBM for modeling industrial flows.


1994 ◽  
Vol 116 (2) ◽  
pp. 332-340 ◽  
Author(s):  
M. Hirota ◽  
H. Fujita ◽  
H. Yokosawa

This paper presents experimental results concerning a time-mean temperature field obtained in forced convection heat transfer for a turbulent flow through a square duct with a ribbed rough bottom wall. The secondary flow pattern in the duct is reflected in the distribution of the local Nusselt number, the values of which on the smooth walls of the rough duct are 1.71~1.97 times those of the smooth duct. In the upper half cross section near the upper smooth wall opposite the bottom ribbed rough wall, the profile of the mean temperature distribution is similar to that of the primary flow velocity distribution, and the validity of the temperature inner law was confirmed. However, in the lower half cross section near the bottom ribbed rough wall, the dissimilarity between the mean velocity and the mean temperature fields becomes pronounced, and the inner law is not valid for mean temperature distributions. The mechanism of the heat transfer near the ribbed rough wall was examined based on the transport equations of turbulent shear stress and turbulent heat flux.


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