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利用柔性涡发生器和串列圆柱增强微通道中幂律流体的传热研究

裴轶尧 管鑫涛 黄静林 王志华 李捷

裴轶尧, 管鑫涛, 黄静林, 等. 利用柔性涡发生器和串列圆柱增强微通道中幂律流体的传热研究[J]. 航空动力学报, 2025, 40(10):20240458 doi: 10.13224/j.cnki.jasp.20240458
引用本文: 裴轶尧, 管鑫涛, 黄静林, 等. 利用柔性涡发生器和串列圆柱增强微通道中幂律流体的传热研究[J]. 航空动力学报, 2025, 40(10):20240458 doi: 10.13224/j.cnki.jasp.20240458
PEI Yiyao, GUAN Xintao, HUANG Jinglin, et al. Study on enhanced heat transfer of power-law fluids in microchannels using flexible vortex generators and tandem cylinders[J]. Journal of Aerospace Power, 2025, 40(10):20240458 doi: 10.13224/j.cnki.jasp.20240458
Citation: PEI Yiyao, GUAN Xintao, HUANG Jinglin, et al. Study on enhanced heat transfer of power-law fluids in microchannels using flexible vortex generators and tandem cylinders[J]. Journal of Aerospace Power, 2025, 40(10):20240458 doi: 10.13224/j.cnki.jasp.20240458

利用柔性涡发生器和串列圆柱增强微通道中幂律流体的传热研究

doi: 10.13224/j.cnki.jasp.20240458
详细信息
    作者简介:

    裴轶尧(1999-),男,硕士生,从事流体力学及对流换热研究

  • 中图分类号: V228.3;TU832.2+3

Study on enhanced heat transfer of power-law fluids in microchannels using flexible vortex generators and tandem cylinders

  • 摘要:

    利用壁挂式柔性涡流发生器(FVG)、串列圆柱和非牛顿流体增强微通道的传热,采用任意拉格朗日-欧拉(ALE)格式的有限元法,对描述微通道中流固耦合的连续性方程、动量方程和能量方程进行求解。在双圆柱间距离固定的条件下,调整FVGs与圆柱之间的间距以及改变流体的幂律指数(n),研究对称壁挂式FVGs通道中幂律流体的流致振动现象及换热性能。与直微通道相比,当下游圆柱与柔性板间距离Gx=1.5、幂律指数n=1.2时,努塞尔数Nu增加了184%,热性能系数增加了45%。

     

  • 图 1  双圆柱诱导对称壁挂式FVGs结构示意图

    Figure 1.  Schematic structure of double columns induced symmetric wall-mounted FVGs

    图 2  称壁挂式 FVGs 网格示意图

    Figure 2.  Schematic diagram of the grid of the wall-mounted FVGs

    图 3  对称壁挂式FVGs上板的Xtip运动历程(20 s≤t≤ 20.2 s)

    Figure 3.  Motion history of Xtip of the upper plate in the symmetric wall-mounted FVGs (20 s≤t≤20.2 s)

    图 4  微通道内涡量场

    Figure 4.  Vorticity field in the microchannel

    图 5  二维参数空间(Gx, n)上两个对称壁挂式FVGs的4种不同摆动模式的区域划分图

    Figure 5.  Regional division of two symmetric wall-mounted FVGs with four different oscillation modes on a two-dimensional parameter space (Gx, n

    图 6  不同模式下的上下板的尾端横向位移、纵向位移的时间历程以及尾端横向位移的功率谱

    Figure 6.  Time histories of the transverse displacement and longitudinal displacement of the tail end of the upper and lower plates and the power spectra of the tail end in different modes

    图 7  Gx, n)=(2.0,1.0)时尾端横向位移Ytip和纵向位移Xtip的时间历程以及Ytip的频谱Pf

    Figure 7.  Time histories of the transverse displacement (Ytip) and longitudinal displacement (Xtip) of the tail end and the power spectra of the tail end YtipPf) for (Gx, n)=(2.0,1.0)

    图 8  O模式下对称壁挂式FVGs周围4个时刻下的涡量场

    Figure 8.  Vorticity fields around symmetric wall-mounted FVGs at four moments in O mode

    图 9  O模式下对称壁挂式FVGs周围4个时刻下的温度云图

    Figure 9.  Temperature clouds around symmetric wall-mounted FVGs at four moments in O mode

    图 10  O模式下上下壁面的(Ⅰ~Ⅳ)时刻瞬时努塞尔数(Nu

    Figure 10.  Instantaneous Nusselt number (Nu) at (I—Ⅳ) moments for the upper and lower walls in O mode

    图 11  20.00 s≤t≤20.50 s时间内几种典型案例下平均Nu($ \overline{Nu} $)的空间变化

    Figure 11.  Spatial variation of mean Nu ($ \overline{Nu} $) for several typical cases at time 20.00 s≤t≤20.50 s

    图 12  带双圆柱的对称FVGs系统整体努塞尔数Nuavg 和阻力系数$ {C}_{\rm{f}} $在(Gx, n)区域内的等高线图

    Figure 12.  Contour plots of the overall Nusselt number Nuavg and total flow resistance coefficient $ {C}_{\rm{f}} $ of the symmetric FVGs with double columns in the (Gx, n) region

    图 13  相较于牛顿流体和相较于直微通道的带双圆柱的对称FVGs的热效率在(Gx, n)区域内的等高线图

    Figure 13.  Contour plots of the thermal efficiency of the symmetric FVGs with double columns compared to the Newtonian fluid and compared to the straight microchannel in the (Gx, n) region

    图 14  对称FVGs、直微通道及带双圆柱的对称FVGs的整体努塞尔数Nuavg、阻力系数$ {C}_{\rm{f}} $和性能评价标准Pec,cm随幂律指数(n)的变化

    Figure 14.  Overall Nusselt number Nuavg, total flow resistance coefficient $ {C}_{\rm{f}} $, and performance evaluation criteria Pec,cm as a function of the power-law exponent (n) for the symmetric FVGs, straight microchannel, and symmetric FVGs with double columns

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出版历程
  • 收稿日期:  2024-07-06
  • 网络出版日期:  2025-03-26

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