2012
DOI: 10.1016/j.ijsolstr.2012.04.023
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Crack onset and growth at the fibre–matrix interface under a remote biaxial transverse load. Application of a coupled stress and energy criterion

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Cited by 53 publications
(29 citation statements)
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“…The materials of both the inclusion and the matrix are considered to be linear, elastic and isotropic. Let (x, y) and (r, θ) be the cartesian and polar coordinates with the origin of coordinates in the center of the inclusion, assuming without any loss of generality that (x, y) is the principal coordinate system of the remote stress state defined by the principal stresses σ ∞ x ≥ σ ∞ y , see Although the ratio of the principal stresses η = σ ∞ y /σ ∞ x = tan φ ∞ is sometimes used to characterize the biaxiality of the remote stress state (Mantič and García 2012), in the present study, which covers also configurations where both remote principal stresses are compressive, the following general load-biaxiality parameter 1 :…”
Section: The Problem Of a Cylindrical Inclusion Under Biaxial Transvementioning
confidence: 99%
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“…The materials of both the inclusion and the matrix are considered to be linear, elastic and isotropic. Let (x, y) and (r, θ) be the cartesian and polar coordinates with the origin of coordinates in the center of the inclusion, assuming without any loss of generality that (x, y) is the principal coordinate system of the remote stress state defined by the principal stresses σ ∞ x ≥ σ ∞ y , see Although the ratio of the principal stresses η = σ ∞ y /σ ∞ x = tan φ ∞ is sometimes used to characterize the biaxiality of the remote stress state (Mantič and García 2012), in the present study, which covers also configurations where both remote principal stresses are compressive, the following general load-biaxiality parameter 1 :…”
Section: The Problem Of a Cylindrical Inclusion Under Biaxial Transvementioning
confidence: 99%
“…The corresponding Dundurs bi-material parameters in plane strain are α = 0.919 and β = 0.229, and the harmonic mean of the effective elasticity moduli is E * = 6.01GPa, see (París et The strength and fracture properties of the fibre-matrix interface, tensile strengthσ c = 90 MPa and fracture energy in mode IḠ Ic = 2 Jm −2 , considered in the numerical procedure are in the range of values found in the literature (Zhang et al 1997;Varna et al 1997) and correspond to quite brittle behaviour (Mantič 2009;Mantič and García 2012), making the hypothesis for the LEBIM represent appropriately a real possible composite material behavior (Távara et al 2011). Then, k n is determined by (6).…”
Section: The Problem Of a Cylindrical Inclusion Under Biaxial Transvementioning
confidence: 99%
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