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Finite element analysis of a subsurface crack on the0 [1 s( x7 b+ R1 ?4 [, S6 d) J0 R
interface of a coateh material under a moving' D( ~- w6 f' U# J: ]& p
compressive load
^% ?; X9 M8 g3 S# |. ^117% G6 L, x* @, u! B0 R( w
K S. Leea**, J. T. Jinn” and Y. Y. Earmmeb; D3 U7 s/ _0 V1 }# K, o, u$ J/ c' Q
“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan
m9 X+ G& \; q2 H# H6 _Gyeongnam, 680-749 Seoul (Korea)
0 y4 T& k" l! S1 ?. z“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology, ^; z9 b2 |9 A8 x9 Q! m
Seoul (Korea)6 i, Z" _$ ~! y, X: t: M1 n: t
(Received July 11, 1991; revised and accepted, October 30, 1991)
, p9 G. B$ T( ?* g/ ]Abstract0 E0 d/ c0 V! T7 w7 Z! q
A subsurface crack subjected to a moving compressive load is analysed with the finite, p9 w9 J' n T/ F3 z4 _' r3 T
element method (FEM) considering friction on the crack surface. By comparing the FEM
% T! ` T; A; ?* U* F! Bresults with semianalytic results of the subsurface crack in a homogeneous medium, it is$ N/ B6 \4 m u2 W3 C8 e
first verified that the present solution method gives a fairly good result. The fracture
" s* E$ B- m: `5 Fparameters for the subsurface crack on the interface of a coated material are then evaluated' J* o5 ]' ^2 w6 \
numerically for various cases such as different combinations of materials of the coating% Y. R) e; K6 s$ @8 m- g0 h" {8 Y
layer and the substrate, changes in the ratio of the length of the subsurface crack to the
4 \8 q" u7 A! s/ }7 [" N% ]: Fthickness of the coating layer and changes in the coefficient of friction on the crack surface.
- a! P4 G* ^6 \; i/ AThe effects of the combination of materials, the geometry of the subsurface crack and the( O( o$ _# O7 [9 J3 U2 B4 l- c
coefficient of friction on the fracture parameters are discussed. The conditions for the
; \3 A: |. n/ W% M) {& csubsurface crack to propagate along the interface or to kink out of the interface are also
9 k6 w1 j1 _9 f3 ]examined. |
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