...
首页> 外文期刊>International Journal of Heat and Mass Transfer >Direct numerical simulation of natural convection in a square cavity with uniform heat fluxes at the vertical sides: Flow structure and transition
【24h】

Direct numerical simulation of natural convection in a square cavity with uniform heat fluxes at the vertical sides: Flow structure and transition

机译:在垂直方向上具有均匀热通量的方腔中自然对流的直接数值模拟:流动结构和过渡

获取原文
获取原文并翻译 | 示例

摘要

Direct numerical simulations have been performed of natural convection in a closed cavity with constant heat fluxes on the vertical sides. Results are presented for Rayleigh numbers in the range 3×10~(11)-4×10~(14) and Prandtl number equal to 1. The flow is characterized by two boundary layers near the heated and cooled vertical sides and two intrusion layers near the horizontal walls, which complete a recircula-tion pattern. The net energy surplus transferred upwards by both boundary layers is balanced by heat conduction through the main body of the cavity. The vertical boundary layer thickness is of O(Ra~(-2/9)) and the intrusion layers of O(Ra~(-1/6)). Scalings for thicknesses, velocities and temperature gradients, obtained from order of magnitude estimates, are confirmed by the numerical simulations. The bulk temperature gradient is much larger than those across the thin boundary layers and, therefore, effective in delaying the onset of instability. Unstable flows are thus found only above a Rayleigh number of the order of 10~(12), in contrast to a cavity with fixed lateral wall temperatures where this is close to 10~8. The threshold for instability and the dominant frequencies are in satisfactory accord with relevant linear stability results from the literature. The bulk of the cavity responds passively and filters the excitation from the unstable boundary layers by retaining frequencies close to the Brunt-Vaisala frequencies in a density stratified fluid.
机译:直接数值模拟已经在垂直方向上具有恒定热通量的封闭腔体中进行了自然对流。给出了在3×10〜(11)-4×10〜(14)范围内的瑞利数和Prandtl数等于1的结果。流动的特征是在加热和冷却的垂直侧附近有两个边界层和两个侵入层在水平壁附近,完成了再循环模式。由两个边界层向上传递的净能量剩余通过通过腔体的热传导来平衡。垂直边界层厚度为O(Ra〜(-2/9)),侵入层的厚度为O(Ra〜(-1/6))。从数量级估计获得的厚度,速度和温度梯度的缩放比例已通过数值模拟得到确认。整体温度梯度比薄边界层的温度梯度大得多,因此有效地延迟了不稳定的发生。因此,与具有固定侧壁温度的腔接近10〜8时相比,不稳定的流动仅在高于10〜(12)量级的瑞利数之上发现。不稳定的阈值和主导频率与文献中相关的线性稳定性结果令人满意。空腔的大部分通过在密度分层流体中保持接近Brunt-Vaisala频率的频率来被动响应并滤除不稳定边界层的激发。

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号