Forced convection for flow across two tandem cylinders with rounded corners in a channel
Forced convection for flow across two tandem cylinders with rounded corners in a channel
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DOI:
10.1016/j.ijheatmasstransfer.2018.10.125
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发表时间:
2019-03
影响因子:
5.2
通讯作者:
Wei Zhang;Xiao-ping Chen;Hui Yang;H. Liang;Yi-kun Wei
中科院分区:
文献类型:
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作者:
Wei Zhang;Xiao-ping Chen;Hui Yang;H. Liang;Yi-kun Wei
This work presents the first numerical investigation on the forced convection of flow across two tandem cylinders with rounded corners in a channel atRe= 100. Both cylinders have the geometry of a square rounded at all corners with a radius of curvatureR, which is non-dimensionalized asR+=R/DwhereDis the cylinder diameter, thus the cylinder geometry can be square (R+= 0.0), partially rounded (R+= 0.1–0.4) or circular (R+= 0.5). The two cylinders are separated at a distance in the streamwise direction as characterized by the parameter of gap ratio (GR) chosen atGR= 1(1)8. The objective of this work is to explore the effects of two significant parameters, i.e., gap ratio and corner radius, on the flow unsteadiness and heat transfer characteristics of the tandem arrangement that has not been studied before. The effects of the two parameters are exhibited and analyzed by the instantaneous temperature and vorticity fields, variation of representative aerodynamic and heat transfer quantities, spatial distributions of local heat transfer rate, flow behaviors in the gap and the near-wake regions, and temperature distribution and variation on the channel wall. The results are presented by time-averaged and fluctuating quantities to reflect both mean and pulsating behaviors. We observed that the cylinder geometry determines the unsteadiness of the near-wake flow after the downstream cylinder; the flow is always unsteady for square-like cylinders where the corner radius is small, while the flow can be stabilized by the circular-like cylinders with larger corner radii that the flow fluctuation is greatly weakened or even fully suppressed at smallGRs. Numerical results also reveal that the gap flow is steady at smallGRs and unsteady at largeGRs, as categorized assteady gap flow regimeandunsteady gap flow regime. There are drastic variations for the representative characteristic quantities at the criticalGRwhere the gap flow transits from steady to unsteady. The different flow regimes categorized byGRandR+also substantially determine the flow patterns in the gap and near-wake regions, the mean and fluctuating of heat transfer rate on the cylinder surface and the temperature variation on the channel wall.