共查询到18条相似文献,搜索用时 125 毫秒
1.
2.
3.
4.
5.
6.
合金凝固过程中存在于枝晶尖端液相区的强制对流和自然对流均能改变溶质扩散层厚度,从而会对枝晶形貌产生较大影响.在元胞自动机模型基础上,耦合液体流动方程、热传导方程和溶质对流扩散方程,建立了新的计算微观组织演化的数值模型,并利用该模型研究了强制对流和自然对流对枝晶生长的影响.三维数值模拟结果再现了强制对流作用下等轴枝晶的生长过程,揭示了强制对流对枝晶生长速率和尖端半径的影响特点.同时利用该模型模拟了NH4Cl-H2O溶液定向凝固过程中自然对流对柱状晶生长的影响,并采用相应的实验进行验证.模拟结果与实验结果符合良好,从而证明该模型是可靠的,可推广到实际合金系中.
关键词:
元胞自动机
对流
4Cl-H2O溶液')" href="#">NH4Cl-H2O溶液
定向凝固 相似文献
7.
8.
9.
在无扰动、随机式扰动以及正弦式扰动下,通过对竖直恒温面处状态Ra为1.328×10^9、Pr为6.24的自然对流进行模拟,探索了热边界层的不稳定性和共振强化自然对流换热。结果表明:(1)竖直自然对流边界层上游位置的随机式扰动对热边界层的影响主要体现在稳定阶段;(2)该状态下的竖直自然对流边界层的特征频率为15 067,且相比于无扰动状态,频率为15 067的正弦式扰动能在竖直恒温面处提高5.15%的换热量;(3)在竖直自然对流边界层上游位置加入特征频率的正弦式扰动,竖直恒温面处的局部努塞尔数Nu均出现明显波动,且波动随着边界层高度的增加而增大。 相似文献
10.
11.
Simulation of natural convection under high magnetic field by means of the thermal lattice Boltzmann method 下载免费PDF全文
The thermal lattice Boltzmann method (TLBM), which was proposed by
J. G. M. Eggels and J. A. Somers previously, has been improved in
this paper. The improved method has introduced a new equilibrium
solution for the temperature distribution function on the assumption
that flow is incompressible, and it can correct the effect of
compressibility on the macroscopic temperature computed. Compared to
the previous method, where the half-way bounce back boundary
condition was used for non-slip velocity and temperature, a
non-equilibrium extrapolation scheme has been adopted for both
velocity and temperature boundary conditions in this paper. Its
second-order accuracy coincides with the ensemble accuracy of
lattice Boltzmann method. In order to validate the improved thermal
scheme, the natural convection of air in a square cavity is
simulated by using this method. The results obtained in the
simulation agree very well with the data of other numerical methods
and benchmark data. It is indicated that the improved TLBM is also
successful for the simulations of non-isothermal flows. Moreover,
this thermal scheme can be applied to simulate the natural
convection in a non-uniform high magnetic field. The simulation has
been completed in a square cavity filled with the aqueous solutions
of KCl (11wt%), which is considered as a diamagnetic fluid with
electrically low-conducting, with Grashof number Gr=4.64×
10^4 and Prandtl number Pr=7.0. And three cases, with different
cavity locations in the magnetic field, have been studied. In the
presence of a high magnetic field, the natural convection is quenched
by the body forces exerted on the electrically low-conducting
fluids, such as the magnetization force and the Lorentz force. From the
results obtained, it can be seen that the quenching efficiencies
decrease with the variation of location from left, symmetrical line,
to the right. These phenomena originate from the different
distributions of the magnetic field strengths in the zones of the
symmetrical central line of the magnetic fields. The results are
also compared with those without a magnetic field. Finally, we can
conclude that the improved TLBM will enable effective simulation of the natural
convection under a high magnetic field. 相似文献
12.
13.
14.
对牛顿流体内溶解双颗粒在垂直管道中的沉降运动进行了直接数值模拟. 流体运动由守恒方程计算, 密度和黏性的变化考虑流场温度变化的影响, 通过积分粘性应力和压力获得颗粒的受力跟踪颗粒运动, 溶解引起的相变及其形状的变化由溶解潜热、溶解质量与分散相边界处的温度梯度的关系建立的方程决定. 通过颗粒和流体间相互的作用力和力矩及边界条件的施加实现相间耦合. 对双颗粒在等温流体无溶解条件和非等温流体溶解条件下的沉降过程进行了计算. 结果表明, 在一定雷诺数内, 热对流产生的颗粒尾迹处涡的脱落以及溶解引起的颗粒质量、颗粒表面形态的变化引起了颗粒的横向摆动, 并使颗粒沉降速度发生了变化. 相似文献
15.
纳米流体作为一种较高的导热介质, 广泛应用于各个传热领域. 鉴于纳米颗粒导热系数和成本之间的矛盾, 本文提出了一种混合纳米流体. 为了研究混合纳米流体颗粒间相互作用机理和自然对流换热特性, 在考虑颗粒间相互作用力的基础上, 利用多尺度技术推导了纳米流体流场和温度场的格子Boltzmann方程, 通过耦合流动和温度场的演化方程, 建立了Cu/Al2O3水混合纳米流体的格子Boltzmann模型, 研究了混合纳米流体颗粒间的相互作用机理和纳米颗粒在腔体内的分布. 发现在颗粒间相互作用力中, 布朗力远远大于其他作用力, 温差驱动力和布朗力对纳米颗粒的分布影响最大. 分析了纳米颗粒组分、瑞利数对自然对流换热的影响, 对比了混合纳米流体(Cu/Al2O3-水)与单一金属颗粒纳米流体(Al2O3-水)的自然对流换热特性, 发现混合纳米流体具有更强的换热特性. 相似文献
16.
17.
对牛顿流体内溶解与热对流对单颗粒在垂直管道中的沉降运动进行了直接数值模拟.流体运动由守恒方程计算,密度和黏性的变化考虑流场温度变化的影响,通过积分黏性应力和压力获得颗粒的受力跟踪颗粒运动,溶解引起的相变及其形状的变化由溶解潜热、溶解质量与分散相边界处的温度梯度的关系建立的方程决定.通过颗粒和流体间相互的作用力和力矩及边界条件的施加实现相间耦合.分别模拟了颗粒在等温流体、热流体、冷流体及颗粒溶解四种情况下的沉降过程.结果表明,在一定雷诺数内,热对流产生的颗粒尾迹处涡的脱落以及溶解引起的颗粒表面形态的变化引起了颗粒的横向摆动,并使颗粒沉降速度发生了变化.
关键词:
溶解
热对流
颗粒两相流
直接数值模拟 相似文献
18.
Abstract Results are presented that illustrate the effect of augmenting or opposing thermal and solutal body forces on the flow, temperature and concentration distributions. For augmenting buoyancy forces, the flow field is very similar to that for a single-component fluid. Multicellular flow patterns are observed for opposing buoyancy forces that depend on the buoyancy parameter. The solutal buoyancy force does not dominate the flow field for all values of opposing body forces, because the solutal gradient is vertical. The concentration gradient affects the natural convection through both the additional buoyancy force and the thermophysical properties of the gas mixture. 相似文献