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Fracture in most ceramic starts from natural cracks with sizes a0 in the order of a few 10 μm introduced during the processing of these materials. A crack in a component starts to propagate when the externally applied stress intensity factor Kappl exceeds the so-called crack-tip toughness KI0. In the absence of an increasing crack growth resistance, the strength σc is exclusively governed by KI0 according to
Many ceramic materials exhibit the effect of an increasing crack growth resistance during crack extension Δa, i.e. a rising R-curve with KR = f(Δa) (Fig. 1a). In cases of a moderately rising R-curve, Eq. 1 remains valid. Only in cases of strongly rising R-curves, the strength is affected. For materials with a sufficiently steep R-curve, stable crack extension follows under increasing load. Failure of the component then occurs when the so-called tangent condition is fulfilled, i.e. when the slope of the applied stress intensity factor Kappl(a) and the R-curve KIR(a) are identical