Although numerical simulation tools are now very powerful, the development of analytical models is very important for the prediction of the mechanical behaviour of line contact structures for deeply understanding contact problems and engineering applications. For the line contact structures widely used in the engineering field, few analytical models are available for predicting the mechanical behaviour when the structures deform plastically, as the classic Hertz’s theory would be invalid. Thus, the present study proposed an elastic-plastic model for line contact structures based on the understanding of the yield mechanism. A mathematical expression describing the global relationship between load history and contact width evolution of line contact structures was obtained. The proposed model was verified through an actual line contact test and a corresponding numerical simulation. The results confirmed that this model can be used to accurately predict the elastic-plastic mechanical behaviour of a line contact structure.
and the State Key Laboratory of Earthquake Dynamics(Grant)
the opening projects from the State Key Laboratory of Explosion Science and Technology(Grant)
the National Natural Science Foundation of China(Grant)
This work was supported by the National Natural Science Foundation of China (Grant Nos. 11602022, and 11727801), the opening projects from the State Key Laboratory of Explosion Science and Technology (Grant No. KFJJ16-05M), and the State Key Laboratory of Earthquake Dynamics (Grant No. LED2016B02).
[1]
R. Jackson, H. Ghaednia, H. Lee, A. Rostami, and X. Wang, in
[2] Mao K., Langlois P., Hu Z., Alharbi K., Xu X., Milson M., Li W., Hooke C. J., Chetwynd D.. Wear, 2015, 332-333: 822 CrossRef Google Scholar
[3] Ren C., Chen J., Pan H., Huang X., Zhu H.. Eng. Failure Anal., 2013, 28: 311 CrossRef Google Scholar
[4] Guler M. A., Adibnazari S., Alinia Y.. Int. J. Solids Struct., 2012, 49: 929 CrossRef Google Scholar
[5] Wen Z., Wu L., Li W., Jin X., Zhu M.. Wear, 2011, 271: 426 CrossRef Google Scholar
[6] Andersson P. B. U., Kropp W.. Wear, 2009, 266: 129 CrossRef Google Scholar
[7] Daves W., Kubin W., Scheriau S., Pletz M.. Wear, 2016, 366-367: 78 CrossRef Google Scholar
[8] Johnson K. L.. P. I. Mech. Eng., 1982, 196: 363 CrossRef Google Scholar
[9]
K. Johnson,
[10]
D. Hills, and D. Nowell,
[11] Jiang Y., Sehitoglu H.. J. Tribol., 1994, 116: 577 CrossRef Google Scholar
[12] Jiang Y., Xu B., Sehitoglu H.. J. Tribol., 2002, 124: 699 CrossRef Google Scholar
[13] Merwin J. E., Johnson K. L.. P. I. Mech. Eng., 1963, 177: 676 CrossRef Google Scholar
[14] Zhao Y. P., Wang L. S., Yu T. X.. J. Adhes. Sci. Tech., 2003, 17: 519 CrossRef Google Scholar
[15] Zhang Y., Zhao Y.. Sens. Actuat. A-Phys., 2011, 171: 381 CrossRef Google Scholar
[16]
Y. Zhao,
[17] Ma S., Pang J., Ma Q., Wang X., Wang H.. Polymer Test., 2013, 32: 461 CrossRef Google Scholar
[18] Hills D. A., Nowell D., Barber J. R.. P. I. Mech. Eng. Part C-J. Mech. Eng. Sci., 2017, 231: 2451 CrossRef Google Scholar
[19] Zhu H., He Z., Zhao Y., Ma S.. Polymer Test., 2017, 63: 118 CrossRef Google Scholar
[20] Ma Q., Liu H., Wang H., Sun L., Ma S.. Polymer Test., 2016, 54: 139 CrossRef Google Scholar
[21]
H. Liu, Q. Ma, and S. Ma, in
Figure 1
Line contact. (a) Schematic of the line contact structure; (b) schematic of the contact area; (c) two-dimensional coordinate system.
Figure 2
(Color online) Contact mechanical behaviour of a polycarbonate line contact structure. (a) Experimental setup; (b) average stress-equivalent strain curve; (c) yield zone evolution in the cross-section of the contact cylinder. The white area in (c) represents the yield zone, where
Figure 3
Global stress-strain curve of the bilinear hardening elastic-plastic material.
Figure 4
(Color online) Description of the elastic-plastic deformation over the contact interface of a line contact structure. (a) Contact area before the structural yield moment; (b) compositions of contact area after the structural yield moment. “Reproduced from
Figure 5
(Color online) Contact width-load curves predicted using Hertz’s theory and the proposed model. The line contact structure consists of a cylinder of
Figure 6
(Color online) Average stress-equivalent strain curve predicted using Hertz’s theory and the proposed model.
Figure 7
(Color online) Stress-strain curves of polyimide extracted from uniaxial test at
Figure 8
(Color online) Line contact test in high-temperature environment. (a) Schematic of the line contact test; (b) high-resolution CCD digital camera system with the temperature environment box; (c) contact deformation of AOI at different loading steps.
Figure 9
(Color online) Mesh distribution and boundary condition in FE simulation of the line contact structure.
Figure 10
(Color online) Contact deformation of a polyimide line contact structure at
Copyright 2019 Science China Press Co., Ltd. 科学大众杂志社有限责任公司 版权所有
京ICP备18024590号-1