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Numerical Simulation of Solidification of Colloids Inside a Differentially Heated Cavity

机译:加热腔内胶体凝固的数值模拟

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Development of the solid-liquid interface, distribution of the particle concentration field, as well as the development of thermosolutal convection during solidification of colloidal suspensions in a differentially heated cavity are investigated. The numerical model is based on the one-fluid mixture approach combined with the single-domain enthalpy porosity model for phase change, and it is implemented in fluent software package. The linear dependence of the liquidus and solidus temperatures with the concentration of the nanoparticles was assumed. A colloidal suspension consisting of water and copper or alumina nanoparticles were considered. In the current investigation, the nanoparticle size selected was 5 and 2 nm. The suspension was solidified unidirectionally inside a square differentially heated cavity that was cooled from the left side. It was found that the solid-liquid interface changed its morphology from a planar shape to a dendritic one as the solidification process proceeds in time, due to the constitutional supercooling that resulted from the increased concentration of particles at the solid-liquid interface rejected from the crystalline phase. Initially, the flow consisted of two vortices rotating in opposite directions. However, at later times, only one counter clockwise rotating cell survived. Changing the material of the particle to alumina resulted in crystallized phase with a higher concentration of particles. If it is compared to that of the solid phase resulted from freezing the copper-water colloidal suspension. Decreasing the segregation coefficient destabilizes the solid-liquid interface and increases the intensity of the convection cell with respect to that of the case of no particle rejection. At slow freezing rates, the resulting crystal phase consisted of lower particle content compared to the case of higher freezing rate.
机译:研究了固液界面的发展,颗粒浓度场的分布以及胶体悬浮液在差热腔中固化过程中热固对流的发展。数值模型基于单流体混合方法,结合单域焓孔隙率模型进行相变,并以流利的软件包实现。假设液相线和固相线温度与纳米颗粒的浓度呈线性关系。考虑了由水和铜或氧化铝纳米粒子组成的胶体悬浮液。在目前的研究中,选择的纳米颗粒尺寸为5和2 nm。悬浮液在方形左侧加热的方形加热腔内单向固化。发现随着固化过程的及时进行,固液界面的形态从平面形状变为树枝状,这是由于结构过冷所致,该过冷是由于固液界面上的颗粒浓度增加而导致的。结晶相。最初,流由两个沿相反方向旋转的涡流组成。但是,在以后的时间里,只有一个逆时针旋转的细胞存活了下来。将颗粒的材料更改为氧化铝会导致结晶相的颗粒浓度更高。如果将其与由铜-水胶体悬浮液冻结得到的固相相比较。相对于没有颗粒排斥的情况,降低偏析系数会破坏固液界面的稳定性并增加对流单元的强度。在较低的冷冻速率下,与较高的冷冻速率相比,所得的结晶相包含较低的颗粒含量。

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