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Finite element analysis of a subsurface crack on the) @9 Z- D0 C7 U# S; m
interface of a coateh material under a moving% S4 V0 _/ m* F. I* B( d6 z
compressive load
# ^& B2 b7 m y8 {+ o( `1177 r- h6 }& ^3 B
K S. Leea**, J. T. Jinn” and Y. Y. Earmmeb
( @4 }& \# |* L X) F- R$ K! e+ M“Department of Mechanical Engineering, University of ULran, San 29, Mugeodong, Namgu, Ulsan; v. M: \4 D4 f+ Y4 H
Gyeongnam, 680-749 Seoul (Korea) U! k0 P! @( t; J$ `0 M! C* N! O
“Department of Mechanical Engineering, Korea Advanced Institute of Science and Technology,
) f+ _/ R! q% N3 r m, bSeoul (Korea)
' Q3 @2 u" q: l% _' ~(Received July 11, 1991; revised and accepted, October 30, 1991)) Z3 F* V8 f+ G* |6 A
Abstract, h! Z- k" l; u( g, B5 N
A subsurface crack subjected to a moving compressive load is analysed with the finite8 V! h2 W9 Q4 @3 X7 p: U9 o) I# F. E
element method (FEM) considering friction on the crack surface. By comparing the FEM& { a+ Z' _# q, l6 C
results with semianalytic results of the subsurface crack in a homogeneous medium, it is
: E+ _$ z/ {9 z; s8 Ifirst verified that the present solution method gives a fairly good result. The fracture$ O7 M0 ~- k5 {
parameters for the subsurface crack on the interface of a coated material are then evaluated/ j+ A y& g* R2 y
numerically for various cases such as different combinations of materials of the coating
4 W2 W$ z) D3 X( r# Olayer and the substrate, changes in the ratio of the length of the subsurface crack to the# y% ]/ ^2 S: }
thickness of the coating layer and changes in the coefficient of friction on the crack surface.
) m" j5 M/ Y3 U, p5 J+ }0 @! A7 _- FThe effects of the combination of materials, the geometry of the subsurface crack and the. A- I3 z7 T! ]: Z2 Y
coefficient of friction on the fracture parameters are discussed. The conditions for the% F& T/ W- Q- D* ?) ]5 v4 r
subsurface crack to propagate along the interface or to kink out of the interface are also& r( Q; H) r) M2 P+ ~" J* [& B
examined. |
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