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Finite element analysis of a subsurface crack on the! E$ ?) e$ F6 x/ [5 S9 T, n9 w
interface of a coateh material under a moving2 h% I# u2 K2 [& x; u, D1 R
compressive load
2 \& s, w2 b+ n7 o0 A. F4 Q- M: n1171 {2 |' K9 n6 y$ I9 |. g6 K
K S. Leea**, J. T. Jinn” and Y. Y. Earmmeb; H: q6 g' O2 B. W
“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan. ? d6 L- x" X% d
Gyeongnam, 680-749 Seoul (Korea)( S% H0 \9 I9 ^9 _& P' A
“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,
, M' W8 m E- B7 n% D8 bSeoul (Korea)
6 t0 Z6 Y/ Q3 B$ }(Received July 11, 1991; revised and accepted, October 30, 1991)( D& {7 U n+ h2 |
Abstract* n- \" a& B+ g1 L( e' L% b) t
A subsurface crack subjected to a moving compressive load is analysed with the finite
: U- M \0 M2 welement method (FEM) considering friction on the crack surface. By comparing the FEM7 Q! T& n; |5 x" \, Q
results with semianalytic results of the subsurface crack in a homogeneous medium, it is5 \ F$ O' c/ n! c
first verified that the present solution method gives a fairly good result. The fracture
; V3 c" P8 O7 [0 Y* ?: a1 n5 z; Wparameters for the subsurface crack on the interface of a coated material are then evaluated: P8 ^- }6 K8 u" }- x/ l
numerically for various cases such as different combinations of materials of the coating, Z$ V X3 c. K- M5 \: q$ u* D2 T1 L
layer and the substrate, changes in the ratio of the length of the subsurface crack to the$ ?& M) g8 A& o2 U; O
thickness of the coating layer and changes in the coefficient of friction on the crack surface.3 H0 X. J8 a3 E4 o
The effects of the combination of materials, the geometry of the subsurface crack and the* I0 k( U' p |; {8 J
coefficient of friction on the fracture parameters are discussed. The conditions for the
, F- P- K% y6 `8 asubsurface crack to propagate along the interface or to kink out of the interface are also! [9 L7 ?% i. H& J
examined. |
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