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Finite element analysis of a subsurface crack on the$ @- n3 X7 G. j) J7 P F1 z
interface of a coateh material under a moving. u8 `) r. l! F* m' I' {/ N+ M: K1 Y( C, v
compressive load
/ S/ m/ c. n. m" j1 ~117
, @# D- J( Z5 w( }0 GK S. Leea**, J. T. Jinn” and Y. Y. Earmmeb5 {/ V( ]( e! k6 l
“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan
& h7 n% z% u$ H' R4 X7 @. `- |. T W" xGyeongnam, 680-749 Seoul (Korea)% R$ [! i0 @0 n+ B4 M# B
“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,, u, Q& T2 h* g6 M1 k
Seoul (Korea); d+ U6 \8 P/ T8 O# y
(Received July 11, 1991; revised and accepted, October 30, 1991), |2 B, H" U N' i- M
Abstract
% G0 @/ F/ f/ `/ j- M n/ g4 ?2 t3 LA subsurface crack subjected to a moving compressive load is analysed with the finite; u8 u8 k, U% q% |3 z' v! c9 ~
element method (FEM) considering friction on the crack surface. By comparing the FEM
, \& g& Q. t# g; R1 i! D( Nresults with semianalytic results of the subsurface crack in a homogeneous medium, it is
/ p3 e' V2 l: S; L) Qfirst verified that the present solution method gives a fairly good result. The fracture
7 _4 ]/ H$ ^' \' {: uparameters for the subsurface crack on the interface of a coated material are then evaluated
8 I9 u8 R+ h5 ]# w- O/ l. v# unumerically for various cases such as different combinations of materials of the coating
5 e% T2 M: \' P( D+ h8 T1 zlayer and the substrate, changes in the ratio of the length of the subsurface crack to the, M1 s2 `7 |6 u m! o$ F0 b6 n9 \
thickness of the coating layer and changes in the coefficient of friction on the crack surface.
; m' W: B/ P4 P( lThe effects of the combination of materials, the geometry of the subsurface crack and the4 Y) L3 _7 x. _7 K% J
coefficient of friction on the fracture parameters are discussed. The conditions for the: q& W5 e# `& U& h; T
subsurface crack to propagate along the interface or to kink out of the interface are also; x* F4 C# T4 }+ H6 T
examined. |
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