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Finite element analysis of a subsurface crack on the
% ?( z. O8 N5 J2 X8 Iinterface of a coateh material under a moving
* W- z5 B. I8 Q# Mcompressive load4 c) F0 D8 |0 v( [0 ?6 u
117
1 R9 W+ G) B# V( S5 ~$ {K S. Leea**, J. T. Jinn” and Y. Y. Earmmeb. H. T! h% Y# y, a/ b0 L
“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan
2 ?: A. P0 \& L$ m$ C8 i$ TGyeongnam, 680-749 Seoul (Korea)
: A- b5 C5 E+ E& X“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,
5 f; Y8 e! U! d! C- U WSeoul (Korea)
- Q" e5 ]- @+ E; w0 p(Received July 11, 1991; revised and accepted, October 30, 1991)6 x: t/ {% k [. t1 @
Abstract) {3 [5 H/ j4 `% B. d& f
A subsurface crack subjected to a moving compressive load is analysed with the finite
" Q$ J) x4 L# U- Helement method (FEM) considering friction on the crack surface. By comparing the FEM
2 n4 T& q5 R# E" O5 n) v: @2 fresults with semianalytic results of the subsurface crack in a homogeneous medium, it is
6 W" \6 X) R4 g3 h2 D/ ufirst verified that the present solution method gives a fairly good result. The fracture9 q) v7 C' K* [# {
parameters for the subsurface crack on the interface of a coated material are then evaluated
7 [2 y, }; {* S% B' @% _numerically for various cases such as different combinations of materials of the coating0 T% ?& p' Q2 q) t& @0 ~* S
layer and the substrate, changes in the ratio of the length of the subsurface crack to the l8 z% v* l3 z! A
thickness of the coating layer and changes in the coefficient of friction on the crack surface.+ r( B+ k* T+ Q! T& V: e3 I
The effects of the combination of materials, the geometry of the subsurface crack and the8 _7 ^! K8 I! R8 D6 l+ g
coefficient of friction on the fracture parameters are discussed. The conditions for the
- T$ m' T9 I5 Lsubsurface crack to propagate along the interface or to kink out of the interface are also2 _" l9 x/ J% [, p; u1 x
examined. |
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