Korayem M H, Khaksar H, Sharahi H J
Robotic Research Laboratory, Centre of Excellence in Experimental Solid Mechanics and Dynamics, School of Mechanical Engineering, Iran University of Science and Technology, Tehran, Iran.
Robotic Research Laboratory, Centre of Excellence in Experimental Solid Mechanics and Dynamics, School of Mechanical Engineering, Iran University of Science and Technology, Tehran, Iran.
Ultramicroscopy. 2019 Nov;206:112808. doi: 10.1016/j.ultramic.2019.06.008. Epub 2019 Jun 28.
Regarding the contact mechanics of smooth nanoparticles, two new geometries, specifically elliptical and cubic are chosen for nanoparticles. The results of elliptical contact simulation show that the JKR theory induces a greater indentation depth in both contact geometries since it includes the adhesion forces. Moreover, the Jamari theory shows a lesser indentation depth because it assumes larger contact area. The results of cubic nanoparticles simulation exhibit a significant difference between the contact of tip and nanoparticle compared to the contact of nanoparticle and surface. This can be attributed to the large contact area between the cubic nanoparticle and the reference surface. The JKR and DMT theories, however, show greater indentation depths in the tip contact with nanoparticle. Furthermore, the Lundberg theory yields the maximum indentation depth in the nanoparticle contact with reference surface. Finally, in order to validate the results, experimental and FEM approaches are incorporated. Concerning the experimental results, a certain number of silver nanoparticles are placed on a polystyrene surface. After obtaining the experimental force-displacement curves, the results of presented models are compared with them. The experimental results indicate that for silver nanoparticles and polystyrene surface, the Hertz theory with 1.11% of error and the JKR theory with 8.7% of error show the best output, respectively. Regarding rough nanoparticles contact, the geometry of roughness are taken as elliptical. Meanwhile, analytical relations are presented to solve force and contact area integrals while noting the problem dimensions. The results of simulation show that the JKR theory yields the highest roughness force, followed by the Hertz and Jamari theories, and regarding rough contact area, the Hertz theory creates the largest contact area, followed by the Jamari and JKR theories. The presented analytical method is compared with numerical results as a means of validation.
关于光滑纳米颗粒的接触力学,为纳米颗粒选择了两种新的几何形状,具体为椭圆形和立方体形状。椭圆形接触模拟结果表明,JKR理论在两种接触几何形状中都导致更大的压痕深度,因为它考虑了粘附力。此外,贾马里理论显示的压痕深度较小,因为它假设接触面积较大。立方体纳米颗粒模拟结果表明,与纳米颗粒和表面的接触相比,尖端与纳米颗粒的接触存在显著差异。这可归因于立方体纳米颗粒与参考表面之间的大接触面积。然而,JKR和DMT理论在尖端与纳米颗粒的接触中显示出更大的压痕深度。此外,伦德伯格理论在纳米颗粒与参考表面的接触中产生最大的压痕深度。最后,为了验证结果,采用了实验和有限元方法。关于实验结果,将一定数量的银纳米颗粒放置在聚苯乙烯表面上。在获得实验力 - 位移曲线后,将所提出模型的结果与之进行比较。实验结果表明,对于银纳米颗粒和聚苯乙烯表面,误差为1.11%的赫兹理论和误差为8.7%的JKR理论分别显示出最佳输出。关于粗糙纳米颗粒接触,粗糙度的几何形状采用椭圆形。同时,在考虑问题尺寸的情况下,给出了解决力和接触面积积分的解析关系。模拟结果表明,JKR理论产生的粗糙度力最高,其次是赫兹理论和贾马里理论,而对于粗糙接触面积,赫兹理论产生的接触面积最大,其次是贾马里理论和JKR理论。作为验证手段,将所提出的解析方法与数值结果进行了比较。