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Vortex Ring Formation within a Spherical Container with Natural Convection

机译:具有自然对流的球形容器内的涡流环形成

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A numerical investigation of the transient, three dimensional, laminar natural convection of a fluid confined in a spherical container is carried out. Initially the fluid is quiescent with a uniform temperature T_i equal to the temperature of the wall of the container. At time t=0, the temperature of the wall is suddenly lowered to a uniform temperature T_w=0. The natural convection, that conducts to a vortex ring formation within the sphere, is driven by a terrestrial gravity force (laboratory gravity) and by the step change in the temperature of the wall. A scaling analysis of a simplified transient, two dimensional model, formulated in the cylindrical coordinate system, provides a qualitative description of the flow in the spherical enclosure, from start up (including the three stages of the transient process: boundary layer development, stratification and cooling-down) to the time at which the system reaches the new thermal equilibrium condition (uniform temperature T_w) without motion. The governing three dimensional Navier-Stokes equations for an incompressible fluid, formulated in the Cartesian coordinate system, have been numerically solved by using the h/p spectral element method. The Rayleigh number is in the range: 1 × 10~3 < Ra < 1.5 × 10~5. The average Nusselt number Nu as a function of time is evaluated at the wall of the container. The results provided by the spectral element method are in agreement with the scaling analysis results for low Ra numbers, Ra < 1 × 10~4. As the Ra number is increased, in the range: 1 × 10~5 < Ra < 1.5 × 10~5, the flow becomes unstable and oscillatory in the stratification stage. The temperature, vorticity and pressure fields for the three stages of the transient process are presented.
机译:对球形容器内流体的瞬态,三维,层流自然对流进行了数值研究。最初,流体以等于容器壁温度的均匀温度T_i静止。在时间t = 0,壁的温度突然降低至均匀温度T_w = 0。传导到球体内涡流环形成的自然对流是由地面重力(实验室重力)和壁温的阶跃变化驱动的。在圆柱坐标系中制定的简化瞬态二维模型的比例分析,从开始(包括瞬态过程的三个阶段:边界层发展,分层和形成)开始,对球形外壳中的流动进行了定性描述。冷却至系统达到新的热平衡条件(均匀温度T_w)而没有运动的时间。通过使用h / p谱元方法,在笛卡尔坐标系中公式化了不可压缩流体的控制三维Navier-Stokes方程。瑞利数在以下范围内:1×10〜3

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