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Three-dimensional numerical simulation of spoke pattern in oxide melt

机译:氧化物熔体中辐条图案的三维数值模拟

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In order to reveal the mechanism of the well-known surface spoke patterns, three-dimensional numerical simulations of LiNbO_3 melt flwo in an open crucible (47 mm ×46 mm~h) were performed by menas of the finite differnece method, The crucible side wall was heated at constant the flux and the bottom was assumed to be adiaboatic. Radition heat loss from themelt surface to the ambient was at a temperautre of T_a. It was found that that the Rayleigh effect alone could not reproduce the spoke patern. However, if the Marangoni effect is taken into account, the numericla resutls could semi-quantitatively explain gthe spoke pttern. A skeries of simulaitns with varoius values fo the temperautre coefficient of surface tenison suggests that the spoke patterns are caused bythe Marangoni instability in the tin thermla boundary klayer near the melt surface. Incipience of the spoke pattern is kapproximately predicted by a critical Maranogi number value Ma_c肨ΔTΖ?μα=57.6 which correspondst of the critical Marangoni number for the incipience of the Marangoni instabiity in an adiabatic horizontal layer with a free slip bottom at a constant temeprautre, where γT=-γ/T is the temeporutre coefficient of surface tension, δ the depth of the thermal boundarylayer beneath the melt surface. ΔT the temperautre drop in the boundary layer, μ the viscosity and α the tehrmal diffusion coefficient of the melt, respectively. A series of simultions suggets that a constant temeprautre boundary condtion at the crucible side wall stabilizes the melt surfacde and the spoke pattern becomes very difficult to appear.
机译:为了揭示众所周知的表面辐条图案的机理,通过有限差分法,在敞口坩埚(47 mm×46 mm〜h)中对LiNbO_3熔体流动进行了三维数值模拟,坩埚侧面以恒定的通量加热壁,并假定其底部为绝热的。从主表面到周围环境的辐射热损失为T_a。发现仅瑞利效应不能再现辐条样式。但是,如果考虑到Marangoni效应,则数值结果可以半定量地解释轮辐模式。一系列具有表面张力的温度系数可变值的模拟物表明,轮辐模式是由熔体表面附近的锡热合金边界层中的Marangoni不稳定性引起的。通过临界Maranogi值Ma_c肨ΔTZΔμα= 57.6近似预测轮辐模式的开始,该临界值对应于绝热水平层中Marangoni失稳开始时的临界Marangoni值,该恒定水平的自由底部在绝热水平层中,其中γT=-γ/ T是表面张力的Temeporutre系数,δ是熔体表面下方的热边界层的深度。边界层中的温度降ΔT,熔体的粘度μ和熔体的热扩散系数α。一系列simultions建议,在坩埚侧壁处恒定的temeprautre边界条件可稳定熔体表面,并且轮辐图案变得非常难以出现。

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