用可见光谱测量HL—1M等离子体的旋转速度

用ＳＫＤ高分辨光谱仪测量系统测量了ＣⅢ、ＣⅡ、ＯⅡ及Ｈａ等谱线辐射的多勒位移,给出了ＨＬ－１Ｍ托卡马克等离子体旋转速度,结果表明：环向旋转速度ｖψ右到２２ｋｍ·ｓ＾－１,角向旋转速度ｖθ在等离子体内部与电子逆磁漂移方向同向,在ｒ＝２２ｃｍ附近转变为离子逆磁漂移方向,存在极大值９．６ｋｍ·ｓ＾－１,氢弹丸注入时角向旋转反向,在接近孔栏处又变为电子逆磁漂移方向。激光吹气注入杂质时,ｖθ减小。低杂波注入     

炉内两相流动和煤粉燃烧的双流体-轨道模型

本文首次用双流体一轨道（连续介质－轨道ＣＴ）模型对大尺寸四角喷燃炉内气粒两相流动及煤粉燃烧进行了模拟。该模型基于欧拉气相方程组、欧拉颗粒连续方程和动量方程以及拉氏颗粒能量和质量变化的方程,对各子模型用ｋ－ε－ｋｐ两相湍流模型,ＥＢＵ－Ａｒｒｈｅｎｉｕｓ湍流燃烧模型,煤粉颗粒的水分蒸发,热解挥发和焦炭燃烧的扩散－动力模型,ＤＯ（离散坐标）辐射模型。采用了将坐标扭转一定角度的方法减小入口射流和网格斜交造成的伪扩散。编制了ＬＥＡＧＡＰ－ＦＵＲＮＡＣＥ－３程序,分别对冷态模型炉内两相流动和大尺寸炉内三维两相流动和煤粉燃烧进行了模拟,并与颗粒轨道（ＳＴ）模型的模拟结果进行了对照。采用ＰＤＰＡ对冷态模型炉内气粒两相流场进行了测量。冷态两相流动的模拟与实验结果的对比表明ＣＴ模型的模拟结果和实验符合较好,ＳＴ模型所得颗粒浓度分布和实验山入较大。热态模拟的结果给出了两相速度,气相温度,组分浓度和壁面热流分布。模拟结果定性合理。模拟结果显示在出口处由于气流旋转,有一局部高温区存在。     

中和颗粒可压缩性颗粒层模型

本文针对可压缩颗粒层建立了二维数值模型.首先利用颗粒层中颗粒间的相互位置关系,建立了每一个颗粒的力平衡方程,获得了每一个颗粒的受力大小,然后提出了颗粒层坍塌判据,在此基础上,建立了描述颗粒层的沉积-压缩-沉积的动态过程的可压缩颗粒层模型,模型计算结果表明,颗粒层压缩现象主要发生在下部区域,过滤速度越高、范德华力越小,颗粒层越易坍塌,并且颗粒层的压降出现了脉动,模型结果符合已知的实验结果.     

变力的两种平均力

在物理过程中,常遇到变力作用的过程,涉及到平均力及有关问题计算．如：ＦΔｔ＝ｍｖ－ｍｖ０．及Ｆｓ＝Ｗ中平均力Ｆ是否为同一概念,下面从一道题的解答谈起：ＯＭＡ如图所示：弹簧振子在水平方向上作简谐振动,小球的质量为０．２５ｋｇ,弹簧的劲度系数为１００Ｎ／ｍ,振幅为０．２ｍ．求：①小球在平衡位置速度大小;②从最大位移到平衡位置弹力对小球做的功（忽略摩擦及弹簧质量）．解法１,从最大位移到平衡位置弹力对小球做的功Ｗ＝Ｆｓ＝１２ｋＡ·Ａ＝１２×１００×（０．２）２＝２Ｊ由动能定理Ｗ＝１２ｍｖ２ｖ＝２Ｗｍ＝…     

驻波声场中圆柱形管道周围颗粒的运动特性

针对圆柱形管道外部的流体与颗粒介质运动问题,提出了结合圆柱周围声辐射力和声流Stokes力的研究方法。从柱体外部声流方程出发,得到影响涡流结构的无量纲参数Rem≥325.27时,外涡最大流速大于内涡最大流速。在此基础上,采用Nyborg的边界滑移速度理论,获得管道外部声流的极限滑移速度,推导得出圆柱附近的声辐射力公式。基于此公式,在理论上推导出颗粒速度为0、声辐射力和声流Stokes力平衡时,颗粒临界直径的表达式。通过对圆柱位于不同位置时,圆柱外部的颗粒运动进行仿真模拟,得到与理论公式相一致的结论:颗粒的临界直径的大小与声波频率有关,当颗粒直径小于临界直径时,声流Stokes力为主导,颗粒随声流运动,颗粒直径大于等于临界直径时,声辐射力为主导,颗粒在声辐射力作用下逐渐向声辐射力的节点聚集。理论与仿真结果表明该方法可用于分析管道外颗粒的分布状态,其研究结果有助于解决电站中换热器的管道结垢、热交换率降低等问题。     

利用激光光梯度力消除气溶胶雾霾粒子的机理研究

针对气溶胶雾霾粒子在大气流中所受力的平衡体系(旋转升力平衡重力, 粒子与粒子之间依靠斥力形成稳定的网状的力平衡体系)的问题, 提出了用激光光梯度力破坏力平衡进而消除雾霾的新机理. 首先, 根据牛顿第二定理, 得到了粒子所受力的非线性方程组, 应用Runge-Kutta 法积分求解了雾霾颗粒在大气流中所受的主要力(空气曳引阻力、范德瓦耳斯斥力、旋转升力)的数值, 成功验证了西安市2013年12月17-25日、2014年2月20-26日两次雾霾检测试验结论: 在雾霾过程中, 粒径在0.5-0.835 μm径段的粒子数浓度增加最明显. 其次, 在雾霾粒子形成的均匀介质中, 计算了激光光梯度力的大小. 研究发现, 激光光梯度力的数量级恒大于雾霾颗粒所受主要力的数量级, 激光光梯度力完全可以破坏雾霾颗粒所受力的平衡体系. 因此, 用激光光梯度力消除雾霾是可行的, 这种新的解决雾霾的方法对人们的实际生活、环保及创建美丽的蓝天具有非常重要的意义.     

大速差射流预燃室煤粉燃烧的颗粒轨道法数值模拟

本文用颗粒轨道模型对流场复杂的二维大速差射流燃烧室内煤粉燃烧进行了数值模拟,给出了包括热态气相流场、温度场和浓度场等在内的各种气相场分布,同时也给出颗粒轨道及其速度、温度、质量等的变化。模拟结果再次揭示了该燃烧室内流动和燃烧的主要物理特征,并着重指出煤粉颗粒在燃烧室内的行为对火焰稳定的重要影响。     

气固两相90°弯管流中静电影响颗粒运动的大涡模拟研究

本文采用欧拉–拉格朗日方法对静电平衡情况下的圆形截面90°弯管中的气固两相湍流流动进行了大涡模拟研究,重点研究了弯管中的饱和静电作用和Prandtl第二类二次流对于颗粒输送的影响。结果表明,模拟得到Reb=58k工况下的90°弯管中的载流相流场计算结果与实验结果吻合良好,弯管中平均二次流速度最大可以达到体积速度的55%,并且二次流对于离散颗粒相的输送影响显著。静电作用对于管道中心区域的颗粒影响较小,但对于近壁面区域的颗粒作用影响较大,加强了近壁面区域颗粒运动的湍泳现象。动力学分析结果表明,在远离壁面的大部分管道中心区域内流动对颗粒的拖曳力主导颗粒的运动。而对近壁面区域内的颗粒,静电力与拖曳力大小相当甚至超过拖曳力,静电力主导了近壁面区域内颗粒的运动。     

加压密相气力输送煤粉颗粒荷电特性研究

介绍了一种非接触式移动颗粒静电测试方法,并在加压密相气力输送实验装置上对质量浓度在128～230 kg/m3,气体表观速度在6～15 m/s条件下的煤粉颗粒荷电特性进行了实验研究.颗粒平均粒径为35.6μm.实验结果表明:粉体颗粒荷电指示值随着颗粒浓度的增加逐步增大,浓度在150～160 kg/m3之间时达到最大值,随后减小;指示值随着气体表观速度的增加而增大,而后趋于饱和值.     

湍流条件下煤粉颗粒群着火特性实验研究

本文搭建了平面火焰携带流反应器系统,研究了不同煤粉条件下煤粉颗粒群湍流射流着火特性。实验表明,湍流射流速度下低挥发份煤着火表现出扩散状暗红色火焰形态;随挥发分含量的增大,火焰亮度增加,并且在一定高度处发展为颗粒群群燃着火。随给粉量的增大,着火延迟呈现先减小后增大的趋势,最佳给粉浓度为0.75~1.00 kg/m~3。随粒径的减小,加热速率更快,挥发分大量析出使得火焰亮度增加;并且颗粒间的相互作用增强,更早出现颗粒群的群燃现象。     

Flow characteristics around a rotating grooved circular cylinder with grooved of different depths

The present paper describes the flow characteristics around a rotating grooved circular cylinder with grooves of different depths. The surface structure of a circular cylinder was varied by changing the depths of 32 arc grooves on the surface. The surface pressure on the cylinder is measured for theRe range of from 0.4×10⁵ to 1.8×10⁵ and for rotations of from 0 to 4500 rpm. The drag coefficient of a grooved cylinder increases as the spin rate ratio α (= rotational speed of the cylinder surface/uniform velocity) increases forRe>1.0×10⁵. As the groove depth increases, the drag coefficient of a grooved cylinder is independent from the spin rate ratio α. The direction of the lift force of a smooth cylinder is opposite to the Magnus force forRe>1.0×10⁵. However, the direction of the lift force of a grooved cylinder is the same as that of the Magnus force for allRe>1.0×10⁵. As the groove depth increases, the increase in the slope of the lift coefficient becomes small. These phenomena are related to the positions of the flow separation points, which are clarified from the pressure distribution and flow visualization by the spark tracing method. In addition, in the present study, the flow around a rotating grooved cylinder is clarified by flow visualization.     

翼型绕流的洛伦兹力控制机理

在翼型上翼面壁面附近流场中形成的流向洛伦兹力,可提升翼型的升力减小阻力,然而制约其推广应用的主要瓶颈是极为低下的控制效率,为提高洛伦兹力的控制效率,需研究其控制机理.以翼型绕流的洛伦兹力控制为例,利用双时间步Roe格式及水槽对其进行数值及实验研究.结果表明:洛伦兹力的控制效果随着来流速度的增加而下降,升力增幅和阻力减幅与来流速度大小呈反比关系,但升力增加和阻力减小的规律不变,都是升力先急剧增加随后缓慢增加,而阻力先急剧减小然后再缓慢增加,基本原因为升力和阻力先受洛伦兹力推力的影响而分别增加和减小,随后洛伦兹力作用增加翼面壁面摩擦力,导致升力减小和阻力增加,流向洛伦兹力还导致翼型壁面压力下降,增加翼型升力和压差阻力;壁面摩擦力导致的升力降幅比壁面压力变化导致的升力增幅小,壁面压力变化起主导作用;洛伦兹力推力对阻力的降幅比压差阻力的增幅大,洛伦兹力推力起主导作用,因此阻力减小.     

Response of force behaviors of a spherical particle to an oscillating flow

Combined multi-direct forcing technique and the immersed boundary method is applied to investigate the response of force behaviors of a fixed spherical particle to an oscillating flow. The influences of the inlet oscillating flow at a mean Reynolds number of 300 with six different oscillating frequencies and three oscillating amplitudes are investigated. Three different zones with different behaviors are identified and the specific behaviors of the drag and the lift coefficients are analyzed. The averaged drag coefficient and the maximum lift force exerted on the particle increase with the increment of the oscillating Reynolds number or the oscillating amplitude. When the frequency of the inlet flow is equal to the natural vortex shedding frequency, the average drag coefficient reaches the maximum value. A linear relation between the gradient of the maximum lift coefficient and the frequency as well as the amplitude of the inlet oscillating flow is observed in certain regime.     

喷动床气固流动特性的三维CFD-DEM数值模拟

开展了柱锥形气固流动特性的CFD-DEM耦合三维数值模拟研究。气相场采用基于欧拉坐标体系的k-ε双方程湍流模型,固相场采用基于拉格朗日坐标体系的DEM直接数值模拟方法,跟踪离散颗粒场的每一个颗粒,考虑颗粒与颗粒(壁面)之间的碰撞力、曳力、重力、Magnus升力、saffman升力。颗粒之间的碰撞采用Hertz-Mindlin无滑移模型计算。模拟对象为柱锥形喷动床,其直径为0.152 m,喷口直径为0.019 m,模拟颗粒数22万,探讨了喷动床中射流随时间的发展,不同气速下床内气固流动结构,以及颗粒速度与颗粒浓度的分布,并与实验数据进行了对比。     

Thermophoresis-Assisted Microscale Magnus Effect in Optical Traps

The Magnus effect, commonly observed on the macroscale, has been considered to be negligible at the microfluidic limit. However, the thermophoretic effect at the microscale leads to a strong lift force that acts on the optically trapped and heated microparticles rotating in a liquid flow. This thermophoresis-assisted Magnus effect is experimentally observed and explained through the inhomogeneity of temperature distribution in the flow around the absorbing microparticles rotated by magnetic forces within the limit of ultralow Reynolds numbers.

     

Viscous Interaction Between a Vortex Tube and a Rotating Spherical Particle

The transient advection of a cylindrical vortex tube in a viscous incompressible flow field and its interaction with a rotating/spinning spherical particle has been investigated numerically at Reynolds numbers in the range of 20≤ Re≤200 for angular velocities of 0≤Ω≤0.5. The effects of vortex parameters such as size, circulation strength and initial position relative to the particle, on the temporal behavior of the lift and drag forces are studied. Vortex‐sphere interactions bring about major changes in the flow field particularly when coupled with particle rotation. It is observed that the forces acting on the particle are significantly influenced during the time that the vortex core is in the vicinity of the particle. The extent of these local changes are about ±30% in the drag coefficient and about ±200% in the lift coefficient as compared to flow over a rotating solid sphere with no vortex interaction. It is also found that a vortex with core radius between one and two particle diameters creates the strongest temporal variations in the lift and drag coefficients. Furthermore, maximum lift variations occur for the vortex‐particle head on collision, while a vortex with an offset distance of about one diameter from the principal flow axis generates the maximum drag variations.     

Forces acting on a stationary sphere in power-law fluid flow near the wall

The analysis and evaluation of the forces acting on the particle in a linear shear flow of power-law fluid (PLF) in the presence of the wall were performed. Using the results of a series of computations for a model problem with a spherical particle near a flat wall in the Reynolds number range of 0?200 and the distance to the wall from 0 to 20 particle diameters, the correlation formulas for calculating the coefficients of drag force and lift force were obtained. Special attention was paid to the behavior of the forces acting on the particle approaching the wall.     

Analysis of the forces acting on the saltating particles in the coupled wind-sand-electricity fields

Based on the theoretical model describing the saltation of sand particles in the coupled wind-sand-electricity fields, the numerical simulations of the forces acting on saltating particles, such as the aerodynamic drag force, Magnus effect, Saffman force and electrostatic force, are analyzed in comparison to the gravity force of the particles in the steady windblown sand movement. Furthermore, the laws of the above forces vary with the friction velocity, the diameter of the sand particle, the initial angular velocity and the lift-off velocity are discussed. Supported by the National Natural Science Foundation of China (Grant Nos. 10772075 and 10772074), the Key Project of the National Natural Science Foundation of China (Grant No.10532040), and the Program for New Century Excellent Talents in University (Grant No. NCET-04-0979)     

Anisotropic stokes drag and dynamic lift on cylindrical colloids in a nematic liquid crystal

We have measured the Stokes drag on magnetic nanowires suspended in the nematic liquid crystal 4-cyano-4'-pentylbiphenyl (5CB). The effective drag viscosity for wires moving perpendicular to the nematic director differs from that for motion parallel to the director by factors of 0.88 to 2.4, depending on the orientation of the wires and their surface anchoring. When the force on the wires is applied at an oblique angle to the director, the wires move at an angle to the force, demonstrating the existence of a lift force on particles moving in a nematic. This dynamic lift is significantly larger for wires with homeotropic anchoring than with longitudinal anchoring in the experiments, suggesting the lift force as a mechanism for sorting particles according to their surface properties.     

通道中串列旋转圆柱的格子Boltzmann-虚拟区域方法的模拟

通过结合格子Boltzmann方法(LBM)和虚拟区域(Fictitiou sDomain)思想,建立格子Boltzmann-虚拟区域(LB-DF/FD)方法.采用两套网格系统,欧拉网格用于流体,拉格朗日网格用于固体.原有的LBM在计算运动固体的受力方面存在数据振荡,LB-DF/FD方法改进了此缺陷.为验证该方法,模拟圆柱绕流、圆形颗粒在无限长通道中平动及在无限大流场中转动三种情况,结果与其他数值解及理论解符合得很好.利用该方法模拟低雷诺数下通道中串列旋转圆柱周围的流场,分析圆柱间距(g)及雷诺数(Re)对流场结构的影响.给出Re=0.001,0.1和10下,0.2≤g≤8.0的流线结构、圆柱升力、阻力以及力矩等数值结果.结果表明,g对流场的结构及圆柱的受力有显著影响,Re对圆柱阻力及Stokes单元数目的影响较大.