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Finite element analysis of a subsurface crack on the
$ L) v- o$ s& ?! l" \2 Ginterface of a coateh material under a moving
* p5 m7 V% h0 P& R; Y5 `compressive load
5 V/ `: V$ a U. z& m5 e$ D1 T117
! A& U; k m& d% C) XK S. Leea**, J. T. Jinn” and Y. Y. Earmmeb
+ P1 `6 `( u- I. S: K“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan" R' `( M! A" _$ V3 ]8 J
Gyeongnam, 680-749 Seoul (Korea)
' V: e6 n; K: O* a1 t5 i! B“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,
% g( F$ V5 m+ ]4 p% N+ FSeoul (Korea)% [) e' [) Q Y+ U
(Received July 11, 1991; revised and accepted, October 30, 1991)- E3 E$ M8 A: A9 G. D2 A( j& Q
Abstract8 }! t e. N6 J# @
A subsurface crack subjected to a moving compressive load is analysed with the finite7 q* |; {6 X; I+ b4 E
element method (FEM) considering friction on the crack surface. By comparing the FEM
1 P' w0 S% R0 ~1 y: K$ {results with semianalytic results of the subsurface crack in a homogeneous medium, it is
8 S7 s" G+ y* p+ [& qfirst verified that the present solution method gives a fairly good result. The fracture+ _4 @) j- w, x7 `
parameters for the subsurface crack on the interface of a coated material are then evaluated
( H. q1 g! `9 h8 M" x) @numerically for various cases such as different combinations of materials of the coating* n, K U: {* _2 {7 v6 w
layer and the substrate, changes in the ratio of the length of the subsurface crack to the9 E% ?0 a+ x. r: m, s. a
thickness of the coating layer and changes in the coefficient of friction on the crack surface.
3 u" N) S! i, r U% U; _The effects of the combination of materials, the geometry of the subsurface crack and the
1 q" j h0 ? w6 j0 }coefficient of friction on the fracture parameters are discussed. The conditions for the) Q s4 h( r, v+ ]5 k1 {
subsurface crack to propagate along the interface or to kink out of the interface are also- R5 C' ?. I8 x9 ~$ T1 M9 b
examined. |
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