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The wedge subjected to tractions proportional to rn: A paradox resolved

✍ 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

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✦ 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.


πŸ“œ SIMILAR VOLUMES


The wedge subjected to tractions: a para
✍ J. P. Dempsey πŸ“‚ Article πŸ“… 1981 πŸ› Springer Netherlands 🌐 English βš– 473 KB

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: a para
✍ T. C. T. Ting πŸ“‚ Article πŸ“… 1984 πŸ› Springer Netherlands 🌐 English βš– 539 KB

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