
中山大学 航空航天学院,深圳,518107
Published:2022
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包芸, 何建超, 方明卫. 大Pr数湍流热对流大尺度环流形态变化特性[J]. 空气动力学学报, 2022, 40(2): 174−181.
BAO Yun, HE Jianchao, FANG Mingwei. Large scale circulation transition in thermal convection with large Prandtl number[J]. 2022, 40(2): 174-181.
包芸, 何建超, 方明卫. 大Pr数湍流热对流大尺度环流形态变化特性[J]. 空气动力学学报, 2022, 40(2): 174−181. DOI: 10.7638/kqdlxxb-2021.0335
BAO Yun, HE Jianchao, FANG Mingwei. Large scale circulation transition in thermal convection with large Prandtl number[J]. 2022, 40(2): 174-181. DOI: 10.7638/kqdlxxb-2021.0335.
大尺度环流是湍流热对流的重要特征之一,为了研究大尺度环流形态的变化特征,本文在大Prandtl数(
Pr
)下,较大的Rayleigh数(
Ra
)范围内对热对流的流动形态进行研究。采用直接数值模拟(DNS)计算二维湍流热对流,对大
Pr
= 10、20的热对流大尺度环流形态进行研究,
Ra
范围是1×10
8
~1×10
12
,同时与
Pr
= 4.3情况进行了对比分析。结果表明:大
Pr
数的热对流大尺度环流存在三种形态,方形、椭圆形和圆形,小
Pr
数只有椭圆形和圆形两种;方形的最大速度点在侧壁附近,椭圆形大尺度环流的最大速度点在椭圆与角涡的相剪切处,圆形的最大速度点随机出现在大尺度环流周长线上;方形到椭圆形的转变是一种渐变,存在过渡点,而椭圆形到圆形是突变;大尺度环流的长短轴之比,方形时在1.0~1.2之间,椭圆形时在1.2以上,而圆形时基本为1;大尺度环流形态变化影响Reynolds数(
Re
)的变化规律:补偿
Re
数变化规律显示,大尺度环流形态由方形渐变为椭圆形时,
Re
数出现小量下降,过渡点出现极小值,由椭圆形突变为圆形时,
Re
数出现间断式大幅下降。
We report a numerical study of large scale circulation (LSC) in two-dimensional turbulent thermal convection with two Prandtl numbers (
Pr
= 10
20) and Rayleigh number (
Ra
) ranging from 1×10
8
to 1×10
12
. To compared with small
Pr
some results at
Pr
= 4.3 are shown in this article. Three patterns of LSC are found at large Prandtl numbers
i.e. square
ellipse and circle
while only the
latter two patterns are found at small Prandtl numbers
<
italic/>. For the classical elliptical LSC
the positions of maximum velocity always appear between the LSC and the corner rolls
and the positions appear randomly in the LSC for the circular LSC. Whereas
the maximum velocities appear near the sidewalls for the square LSC. The LSC transition from square to ellipse is a gradual change while the transition from ellipse to circle is a drastic change. The ratio between the major axis and the minor axis of LSC is 1.0~1.2 for square
greater than 1.2 for ellipse
but near 1.0 for circle. The relationship between Reynolds number (
Re
) and
Ra
is influenced by the transition of LSC
which can be indicated by the compensated
Re
. The compensated
Re
decreases slightly and then reaches a local minimum when the LSC changes from square to ellipse
while it decreases sharply from ellipse to circle.
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