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Finite element analysis of a subsurface crack on the
) t4 ]9 g* ?, t) u6 F9 _interface of a coateh material under a moving
! v. j& O, U6 L, i& [0 Acompressive load
! n( o: d6 H' A- W117
! S6 P% b; W6 v9 r+ Q, Q: W" TK S. Leea**, J. T. Jinn” and Y. Y. Earmmeb
% `4 |. m0 }9 @0 I“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan Y5 W! i$ e7 }( ]# [- C; Z
Gyeongnam, 680-749 Seoul (Korea) y( K2 h- Q) p( A7 D2 N
“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,
9 m) `7 \! b9 d" oSeoul (Korea)
* m/ ^5 U! R- e7 n(Received July 11, 1991; revised and accepted, October 30, 1991)% a, V' Q. l" [) V4 N4 k9 L3 A1 Q1 D/ t
Abstract
* ^3 j' j2 A- ?7 z) JA subsurface crack subjected to a moving compressive load is analysed with the finite
, v" m# G- j' r5 m+ E X& Relement method (FEM) considering friction on the crack surface. By comparing the FEM
2 C0 e" h. N% c( Q% ?results with semianalytic results of the subsurface crack in a homogeneous medium, it is( Q' X, X" o: s: N/ j9 n
first verified that the present solution method gives a fairly good result. The fracture
( \& p3 K$ M( v2 A; M6 E3 \# `7 hparameters for the subsurface crack on the interface of a coated material are then evaluated
7 W, w& Y" m8 f) D8 b8 z; Z2 A: O Znumerically for various cases such as different combinations of materials of the coating u7 }8 b" I8 z; O" w" L
layer and the substrate, changes in the ratio of the length of the subsurface crack to the: ^' n( r5 }% @. H. Y6 v) ^
thickness of the coating layer and changes in the coefficient of friction on the crack surface.
! q$ v# a! R' O# Z# P! `8 tThe effects of the combination of materials, the geometry of the subsurface crack and the
5 |& u' j8 D' V( ccoefficient of friction on the fracture parameters are discussed. The conditions for the: w2 J2 i, P h
subsurface crack to propagate along the interface or to kink out of the interface are also3 d, Y9 f% Y5 s U- H/ n8 A- ^
examined. |
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