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Finite element analysis of a subsurface crack on the
9 K9 h( |4 L6 R) t. Jinterface of a coateh material under a moving
& F3 j' x! f9 Ccompressive load& Q# f& J2 Z( O% D
117* O2 s0 r s! e) t! j! h: b2 ]
K S. Leea**, J. T. Jinn” and Y. Y. Earmmeb
0 G( x8 T& v( g6 G0 T“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan
0 _9 X( c. A4 L( h5 O: nGyeongnam, 680-749 Seoul (Korea)$ r& F/ {5 y- S |7 |( Y0 q4 d
“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,/ Z, A1 C1 v0 C# ^. H' g' [! ]
Seoul (Korea)
6 \5 z0 E6 T/ F( b; i(Received July 11, 1991; revised and accepted, October 30, 1991)6 t I% |' G* C2 I( Z
Abstract
* v: B" E9 @2 U/ J- F8 G9 h$ @A subsurface crack subjected to a moving compressive load is analysed with the finite
: N& m8 [8 H4 ?( ?' b- Felement method (FEM) considering friction on the crack surface. By comparing the FEM4 @) P$ }# k' y# |
results with semianalytic results of the subsurface crack in a homogeneous medium, it is/ G0 }/ D5 z9 ~6 a% v8 m2 X6 J
first verified that the present solution method gives a fairly good result. The fracture
( X2 c* M9 J' \8 wparameters for the subsurface crack on the interface of a coated material are then evaluated
: ?; N- C. o9 n- ?& v5 i' H6 \4 Hnumerically for various cases such as different combinations of materials of the coating! O( J. g% N$ p) B" [7 O/ _
layer and the substrate, changes in the ratio of the length of the subsurface crack to the
0 j2 N2 H: Z& }* t0 U& t2 ethickness of the coating layer and changes in the coefficient of friction on the crack surface.
; G8 m8 E) A3 w8 P; T7 D( @The effects of the combination of materials, the geometry of the subsurface crack and the# f8 ~3 b* G: C6 J
coefficient of friction on the fracture parameters are discussed. The conditions for the% Q; a) D) {' g0 }, C" I
subsurface crack to propagate along the interface or to kink out of the interface are also6 K' A& A0 g. C
examined. |
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