Abstract
A boundary-collocation method has been employed to determine the Mode II stress-intensity factors for a pair of through-the-thickness edge cracks in a finite isotropic plate. An elastostatic analysis has been carried out in terms of the complete Williams stress function employing both even and old components. The results of the numerical analysis were verified by a two-step procedure whereby the symmetric (Mode I) and antisymmetric (Mode II) portions of the solution were independently compared with existing solutions. Since no previous analytical solutions existed for the asymmetric loading of an edge-cracked plate, the complete solution was verified by comparison with a photoelastic analysis.
A compact shear (CS) specimen of Hysol epoxy resin was loaded in a photoelastic experiment designed to study the isochromatic-fringe patterns resulting from the Mode II crack-tip stress distribution. The experiment verified that a pure mode II stress distribution existed in the neighborhood of the crack tips, and confirmed the accuracy of the boundary-collocation solution for the Mode II stress-intensity factors. Specimen center-line stress-distribution data were obtained photoelastically and employed to refine the boundary-collocation analysis. Agreement between the analytically and experimentally determined Mode II stress-intensity factors was excellent.
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Abbreviations
- a :
-
notch depth, cm
- B 2,n ,C 2,n :
-
coefficients of the even stressfunction (opening mode) series associated with thenth eigenvalue
- B 4,n ,C 4,n :
-
coefficients of the odd (sliding-mode stress-function series associated with thenth eigen-value
- b, B :
-
specimen thickness, cm
- E :
-
modulus of elasticity, Pa
- f :
-
nondimensinoalized stress-intensity factorK II/σa 1/2
- F σ :
-
material fringe constant, N/fr-m
- h, H :
-
compact-shear-specimen quarter-width, cm
- K,K I,K II,K III :
-
stress-intensity factor at the crack tip, subscript refers to mode of crack extension, Pa m1/2
- K I c,K II c,K III c :
-
critical value of stress-intensity factor at point of instability of crack extension, Pa m1/2
- m :
-
m-th term in eigenfunction expansion
- N, n :
-
refers to thenth eigenvalue of the series expansion for the stress function-number of boundary stations; also refers to fringe order
- \(\bar n\) :
-
refers to the outward unit normal vector drawn on the specimne boundary
- P :
-
applied load; also total (elastic and plastic) work required to extend a crack, N
- r, θ:
-
polar-coordinate directions with origin located at crack tip
- t :
-
symbol for specimen thickness (photoelastic analysis), cm
- w :
-
specimen length (for compact shear specimens) specimen width (for compact tension specimens)
- X, Y, Z, x, y, z :
-
cartesian-coordinate directions
- λ n :
-
nth eigenvalue for the Williams stress function
- σ:
-
boundary stresses applied to compact shear specimens and compact tension specimen =P/BH, Pa
- σ c :
-
critical fracture stress, Pa
- σ r , σθ, σ z , τ r θ:
-
components of the stress tensor in polar coordinates, Pa
- σ x , σ y , σ z :
-
components of the stress tensor, cartesian coordinates, Pa
- σ ys :
-
tensile yield stress, Pa
- σ 1 , σ 2 :
-
principal stresses, Pa
- τ:
-
shear stress applied to tangs of compact shear specimen =KP/BH, Pa
- τ m :
-
maximum in-plane shear stress, Pa
- X :
-
Williams stress function (x=x I+x II), N
- X I :
-
stress function for the stress-free (or zero-displacement) crack surface, N
- X IE :
-
even stress-function component ofX I, N
- X IO :
-
odd stress-function component ofX I, N
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Chisholm, D.B., Jones, D.L. An analytical and experimental stress analysis of a practical mode II fracture test specimen. Experimental Mechanics 17, 7–13 (1977). https://doi.org/10.1007/BF02324265
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DOI: https://doi.org/10.1007/BF02324265