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Finite element analysis of a subsurface crack on the
* k8 f* t6 v r1 D) M. pinterface of a coateh material under a moving
" O1 A0 J) z9 p$ rcompressive load0 A/ h6 j( c) `0 D& u4 c8 h
117
; K$ K# W. d4 a2 i, `* IK S. Leea**, J. T. Jinn” and Y. Y. Earmmeb6 f$ n: Y& l# ~5 N" j
“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan
7 v+ b% h1 J0 x) gGyeongnam, 680-749 Seoul (Korea)
9 b9 j V, r0 `) {“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,( K* c$ T0 p$ T/ Z: @" H- P9 H. t1 p: ?
Seoul (Korea)
. [" w. _* e, e; R- a9 `(Received July 11, 1991; revised and accepted, October 30, 1991): V, g, _3 F- f" I9 J9 |+ R$ g
Abstract
9 [+ B% p1 F" s" I0 LA subsurface crack subjected to a moving compressive load is analysed with the finite. ]; d- \2 s+ D: Y* z3 Y( ]
element method (FEM) considering friction on the crack surface. By comparing the FEM
+ u' B3 o6 y, K; X6 c% gresults with semianalytic results of the subsurface crack in a homogeneous medium, it is
I( o8 C: K( f b5 s9 Afirst verified that the present solution method gives a fairly good result. The fracture2 t0 F6 V/ M2 X
parameters for the subsurface crack on the interface of a coated material are then evaluated; q+ T) o; D6 ^* m: ]. A
numerically for various cases such as different combinations of materials of the coating$ }: y* e" j- Y! W1 q
layer and the substrate, changes in the ratio of the length of the subsurface crack to the
+ L. n) e! X: L$ b% ithickness of the coating layer and changes in the coefficient of friction on the crack surface.' q: ?. Z& e) C6 G1 r- i
The effects of the combination of materials, the geometry of the subsurface crack and the( J" q+ s7 _+ o, c9 x( t0 g
coefficient of friction on the fracture parameters are discussed. The conditions for the
9 Y- ?& `) { r: M7 lsubsurface crack to propagate along the interface or to kink out of the interface are also
/ ^0 K3 h$ n/ \8 |) ~7 cexamined. |
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