首页> 外文会议>International Symposium on Multiphase Flow, Heat Mass Transfer and Energy Conversion >Numerical Simulation of Transient Process of Double-diffusive Convection in a Vertical Circular Cylinder
【24h】

Numerical Simulation of Transient Process of Double-diffusive Convection in a Vertical Circular Cylinder

机译:垂直圆柱内双扩散对流瞬态过程的数值模拟

获取原文

摘要

The transient processes of double-diffusive convection induced by buoyancy force in a vertical circular cylinder have been simulated numerically. Initially, the fluid in the cavity is homogeneous and the top and bottom walls are insulated, then constant temperature and concentration are imposed along the sidewall. The evolution of double-diffusive convection is investigated for specific parameters which are the Prandtl number Pr=7, the Lewis Number Le=5, the thermal Grashof number Gr_T=10~7, the buoyancy ratio N = 1, and the aspect ratio A = 2 for the enclosure. It is compared with nature convection driven by the temperature or solute buoyancy alone. The results show that the flow in the cavity is enhanced and the speeds of evolution of thermal and solutal field increase due to the thermal buoyancy and solutal buoyancy operating simultaneously. Contrasting to the thermal and solutal convection in the quasi-steady stratification state, the isothermal and isoconcentration lines aren't horizontal anymore for double-diffusive convection in that state. In the initial stage, the shape of time traces of temperature, concentration and velocity for double-diffusive convection are similar to those for thermal convection for sake of larger thermal diffusivity (Le=5). At the same time, the results show that the rates of heat and mass transfer at sidewall increase contrasting to those for thermal and solutal convection, respectively.
机译:数值模拟了垂直圆柱体中浮力引起的双扩散对流的瞬态过程。最初,空腔中的流体是均匀的,并且顶壁和底壁是绝缘的,然后沿侧壁施加恒定的温度和浓度。研究了Prandtl数Pr = 7,Lewis数Le = 5,热Grashof数Gr_T = 10〜7,浮力比N = 1和长宽比A等特定参数的双扩散对流的演变。 = 2(对于机柜)。将其与仅由温度或溶质浮力驱动的自然对流进行比较。结果表明,由于热浮力和溶液浮力的同时作用,腔体中的流动得到了增强,而热溶液和溶质场的演化速度加快了。与准稳态分层状态下的热对流和稀释对流相反,在该状态下,双扩散对流的等温线和等浓度线不再是水平的。在初始阶段,由于较大的热扩散率(Le = 5),双扩散对流的温度,浓度和速度的时间迹线形状类似于热对流的时间迹线。同时,结果表明,侧壁的传热和传质速率分别与热对流和溶液对流相反。

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