共查询到19条相似文献,搜索用时 62 毫秒
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用落球法测液体粘度计时起点的确定 总被引:4,自引:0,他引:4
根据斯托克斯定律和牛顿第二定律导出了小球到达终极速度半,小球的运动距离与速度之间的函数关系,从理论上对计时起点的确定给予了证明,并讨论了小球半径的合理取值。 相似文献
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分析了斯托克斯定律及其修正项的适用范围,讨论了落球法测液体粘滞系数实验中液体粘滞系数和落球直径对雷诺数的影响,从理论上给出了实验中落球进入液体后匀速运动的判据. 相似文献
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利用流体力学的知识对小球下落计时起点的确定进行理论推导, 并给出了达到终极速度之前小球运动
的距离与速度之间的函数关系, 以及不同半径的小球达到终极速度时其半径与下落距离的关系 相似文献
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根据落球法测定液体粘滞系数的原理,当重力、浮力和阻力三力达到平衡时,小球匀速下落。对于不同的液体,小球达到匀速的时间和下落的距离并不相等,如果小球未达到匀速就开始计时,测量结果误差将会很大。如果液体粘滞系数太小,斯托克斯公式就不成立了,需要做一个修正。本文就这两个问题进行了讨论,分析出落球法测定液体粘滞系数的适用范围。 相似文献
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落球法测液体粘滞系数实验的改进──双球升降法麻福厚(新疆八一农学院乌鲁木齐830052)用斯托克斯公式测定液体的粘滞系数(粘度)构思巧妙,设备简单.在物理实验教学中独辟蹊径,值得完善与发展.雷诺数是层流转变为湍流的一个数据,自然也是斯托克斯公式的条件... 相似文献
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用落球法测粘滞系数的二级近似公式,有些教材是以过时的戈尔茨坦(Goldstein)公式为依据得出来的,而雷诺(Reynolds)数R~2项的系数却与原公式不一致。本文提出一些商榷意见,并讨论一下落球法的使用范围。一、正确的二级近似公式直径为d的小球,在粘滞系数为η、 相似文献
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根据泊肃叶公式的积分形式,得到了泊肃叶公式的求和形式,从而导出了液体粘度的理论修正公式,比较了理论修正公式与经验修正公式,并提出了小球半径与管半径之比的合理取值。 相似文献
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Measurement of diffusion coefficient of transparent liquid solutions using Michelson interferometer 总被引:1,自引:0,他引:1
V.K.Vani K. Chhaniwal Arun Anand C. S. Narayanamurthy 《Optics and Lasers in Engineering》2004,42(1):9-20
The study of diffusivity is important for the design of chemical equipment and its knowledge is needed for mass transfer studies and is the most fundamental property of any chemical system in which the chemical engineers are interested. Here, we report a new interferometric technique to determine the diffusion coefficient of transparent liquid solutions using Michelson interferometer geometry. The experimental cell containing the diffusing solution was kept in one of the arms of Michelson Interferometer. The liquids of differing concentrations were introduced in the cell. Two separate circular interference fringe systems were formed due to the two solutions and they were recorded on a PC using a CCD camera. The time variation of these interferograms yields the diffusion coefficient. The obtained diffusivity values matched very well with the existing experimental results. Detailed theoretical and experimental analysis is given in the paper. 相似文献
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Three-dimensional wave processes in vertically falling films of viscous liquid are considered. The 3D localized perturbations,
which are studied insufficiently, are of a particular interest. The numerical method for watching evolution of initial perturbations
was developed. The final stage of this evolution is formation of the 3D localized structures: solitons. The boundaries of
3D soliton stability were determined. 相似文献
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《中国光学快报(英文版)》2016,(4)
We report the measurements of Brillouin gain coefficients in FC-770, FC-40, FC-43, and FC-70 using a Brillouin oscillator and amplifier system. In contrast to the traditional way, the novel method provides direct measurements of these coefficients with the medium electro-strictive coefficient or with the phonon lifetime absent. Additionally, the Brillouin gain coefficient of FC-70 in this experiment is different from the theoretical work. 相似文献
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O. Yu. Tsvelodub 《Thermophysics and Aeromechanics》2012,19(1):91-99
Evolution of disturbances on the surface of liquid film falling free over a vertical plane is considered. In the case of low Reynolds numbers, the problem is reduced to investigation of a single equation describing evolution of film thickness disturbances. With the use of information about the structure of the family of steady-state traveling solutions to this equation, the typical scenarios of evolution for periodic disturbances were identified. 相似文献
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设计了一种塑料靶表面涂铋(Bi)的靶丸替代常规内爆靶,利用分幅相机获取辐射驱动内爆替代靶丸Bi等离子体再发射X射线的2维图像。实验时,从主激光中分出一束光信号,经光电转换后作为分幅相机的触发信号,以激光直接驱动金球靶建立相机的时标。根据分幅相机的时标可确定每幅X射线图像相对于主激光的时间延迟。分析Bi球靶的X射线分幅图像,得到夹持内爆靶丸的CH膜的烧蚀时间及Bi球靶半径的变化关系。通过X射线图像还可反推出诊断孔的大小和CH膜支撑靶丸的对称性。 相似文献
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The flows of viscous liquid film over the outer surface of a vertical cylinder are examined. Investigation of wave regimes in the case of low flow rates and large cylinder radii is reduced to the analysis of solutions to a nonlinear evolution equation for the film thickness. There are countable numbers of steady-state traveling solution families in the considered model. In turn, most of them are unstable to 2D and 3D perturbations. Thus, evolution of initial perturbations in different ranges of parameter values differs significantly. Some typical scenarios of perturbation development are presented in this work. Initial perturbations with some symmetries, kept in the process of evolution, are of a particular interest. In these cases, solutions are drawn up to the steady-state traveling solutions with similar symmetry. 相似文献