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By Fowles G.R., Cassiday G.L.

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38) The characteristic of the stress field, namely the power λ in Eq. 33, is dependent not only on the combination of material but also on the shape of the edge (the angles of materials 1 and 2 near the interface edge, ϕ1 and ϕ2 ). λ = 1 − p, which is evaluated by Eq. 34, is not equal to 1/2 in general. The singularity appears in 0 < p < 1, while it does not in 1 < p. It should be noted that Eq. 34 sometimes has two solutions, which means the combined singularity appears in the vicinity of the interface edge.

Reedy, E. , Jr. (1993) Free-edge stress intensity factor for a bonded ductile layer subjected to shear, J. Appl. , 60, pp. 715–720. Rice, J. R. (1968a) A path independent integral and the approximate analysis of strain concentration by notches and cracks, Trans. ASME, J. Appl. , 35, pp. 379–386. Rice, J. R. (1968b) Mathematical analysis in the mechanics of fracture, in Fracture (ed. ), Vol. 2, pp. 191–311, Academic Press, New York. Rice, J. , and Rosengren, G. F. (1968) Plane strain deformation near a crack tip in a power-law hardening material, J.

154–161. , and Komatsu, T. (1979b) Application of J-integral to high-temperature crack propagation. Part II: fatigue crack propagation, Trans. ASME, J. Eng. Mater. , 101, pp. 154–161. , and Ohtani, R. (1995) Delamination behavior of a carbon-fiber-reinforced thermoplastic polymer at high temperatures, Comp. Sci. , 53, pp. 333–341. Wang, T. C. (1990) Elastic-plastic asymptotic fields for cracks on biomaterial interfaces, Eng. Fract. , 37, pp. 527–538. , and Mutoh, Y. (2002) A method for determining elastic-plastic stress singularity at the interface edge of bonded power law hardening materials, JSME Int.

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