The classical two-dimensional solution provided by L6vy for the stress distribution in an elastic wedge, loaded by a uniform pressure on one face, becomes infinite when the opening angle 2c~ of the wedge satisfies the equation tan 2c~, = 2~,. Such pathological behavior prompted the investigation in
The wedge subjected to tractions proportional to rn: A paradox resolved
β Scribed by Ding Haojiang; Peng Nanling; Li Yu
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 1008 KB
- Volume
- 35
- Category
- Article
- ISSN
- 0020-7683
No coin nor oath required. For personal study only.
β¦ Synopsis
The classical two-dimensional solution for the stress distribution in an elastic wedge subjected to tractions proportional to r"(n/> 0) becomes infinite when the wedge angle 2c~ and the constant n satisfy the definite relations, this is a paradox. For n = 0 it was resolved by Dempsey [Journal of Elasticity l 1, 1-10 ( 1981 )] and Ting [Journal of Elasticity 14, 235-247 ( 1984)], for n > 0 and 2~ = it or 2~ it was resolved by Wang [Acta Mechanica Sinica 18(3), 242-252 (1986)]. However, the above investigations provided only a little resolution of it. In this paper all the cases of the paradox have been studied by employing the complex variable method, and the corresponding bounded solutions are obtained. Moreover, the secondary paradox is discovered in the problem, i.e.. the initial solution for the paradox is still infinite for some special values of (n, 7), and this is also resolved here. From the results obtained it can be observed that the stress distribution contains a/'(In r) term for the paradox and a r"(ln r) 2 term more for the secondary paradox.
π SIMILAR VOLUMES
The classical two-dimensional sohit~on for the stress distribution in an elastic wedge loaded by a uniform pressure on one side of the wedge becomes infinite when the wedge angle 2a satisfies the equation tan 2a. = 2a.. This paradox was resolved recently by Dempsey who obtained a solution which is b