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                       FIGURE 6.31 The microcrack toughening mechanism. The formation of microcracks in or near second-phase
                       particles results in release of strain energy (modulus work) and residual microcrack opening (dilatational
                       work). Taken from Evans, A.G., “The New High Toughness Ceramics.” ASTM STP 1020, American Society
                       for Testing and Materials, Philadelphia, PA, 1989, pp. 267–291.

                          This mechanism is relatively ineffective, as Table 6.1 indicates. Moreover, the degree of micro-
                       crack toughening is temperature dependent. Thermal mismatch and the resulting residual stresses
                       tend to be lower at elevated temperatures, which implies less dilatational strain. Also, lower residual
                       stresses may not prevent the microcracks from becoming unstable and propagating through the
                       particle–matrix interface.
                       6.2.2  TRANSFORMATION TOUGHENING

                       Some ceramic materials experience a stress-induced martensitic transformation that results in shear
                       deformation and a volume change (i.e., a dilatational strain). Ceramics that contain second-phase
                       particles that transform often have improved toughness. Zirconium dioxide (ZrO ) is the most
                                                                                          2
                       widely studied material that exhibits a stress-induced martensitic transformation [42].
                          Figure 6.32 illustrates the typical stress-strain behavior for a martensitic transformation [42].
                       At a critical stress, the material transforms, resulting in both dilatational and shear strains. Figure 6.33(a)
                       shows a crack-tip process zone, where second-phase particles have transformed.
                          The toughening mechanism for such a material can be explained in terms of the work argument:
                       energy dissipation in the process zone results in higher toughness. An alternative explanation is
                       that of  crack-tip  shielding, where the transformation lowers the local crack driving force [42].
                       Figure 6.33(b) shows the stress distribution ahead of the crack with a transformed process zone.













                                                               FIGURE 6.32 Schematic stress-strain response of a
                                                               material that exhibits a martensitic transformation at
                                                               a critical stress.
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