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黄文彬, 李红艳, 徐泳. 填隙幂率流体下两刚性圆球相对错移时的粘性阻力[J]. 力学学报, 2004, 36(1). DOI: 10.6052/0459-1879-2004-1-2002-232
引用本文: 黄文彬, 李红艳, 徐泳. 填隙幂率流体下两刚性圆球相对错移时的粘性阻力[J]. 力学学报, 2004, 36(1). DOI: 10.6052/0459-1879-2004-1-2002-232
ON TANGENTIAL INTERACTION BETWEEN TWO RIGID SPHERES WITH INTERSTITIAL POWER-LAW FLUID[J]. Chinese Journal of Theoretical and Applied Mechanics, 2004, 36(1). DOI: 10.6052/0459-1879-2004-1-2002-232
Citation: ON TANGENTIAL INTERACTION BETWEEN TWO RIGID SPHERES WITH INTERSTITIAL POWER-LAW FLUID[J]. Chinese Journal of Theoretical and Applied Mechanics, 2004, 36(1). DOI: 10.6052/0459-1879-2004-1-2002-232

填隙幂率流体下两刚性圆球相对错移时的粘性阻力

ON TANGENTIAL INTERACTION BETWEEN TWO RIGID SPHERES WITH INTERSTITIAL POWER-LAW FLUID

  • 摘要: 湿颗粒离散元模型以两球作用时填隙流体定常流动解为基础,其中切向作用是难点,国外仅有Goldman的牛顿流体渐近解. 基于Reynolds润滑理论导出了两刚性球切向错动时填隙幂律流体的压力方程,并利用傅立叶级数展开简化,通过数值解法得到相应的压力分布、黏性阻力及阻力矩. 该方程的解较之作者先前对速度场附加假定的结果精确,而当幂指数为1时等价于Goldman的牛顿流体渐近解.

     

    Abstract: Discrete Element Modeling for wet particle assembly is based on the interactionsbetween two spheres with an interstitial fluid, when the fluid behaves as non-Newtonian, theanalysis for the tangential interaction becomes much more complicated. Up-to-date there is onlyGoldman's asymptotic solution for Newtonian fluid.In the authors' previous study, an approximate approach for the tangential interaction with aPower-law fluid was proceeded with an additional assumption for velocity, correspondingly anpressure equation was obtained and then solved numerically to get the viscous force and moment.However, its validity has not yet been estimated.In order to get the more accurate expressions, a new approach was carried out based onReynolds lubrication theory without the additional assumption. As a result a pressure equationwas derived and then simplified by using Fourier-series expansion, after the pressure equationwas solved, corresponding results for the viscous force and moment were obtained. Thenumerical results from the proposed equation were compared with those from the previousequation, showing that the additional assumption could be satisfied automatically for aNewtonian fluid, therefore the previous solutions can be applied to a Newtonian-like Power-lawfluid, otherwise the proposed pressure equation is necessary. For a Power-law fluid, the powerindex is a key factor affecting the accuracy. The more deviation of the index from 1, the moreerrors produced. Generally the differences of viscous force and moment between the previousand the proposed schemes are significant less than those of the pressure distribution.Especially when the power index approaches or exceeds 0.8, the previous results are ingood coincidence with the proposed ones, which suggest that the previous is valid with asatisfied accuracy, in this case, the additional assumption could be taken to simplify thederivation.

     

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