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348                                             Chapter 8  Fracture of Cracked Members


            value of the factor K I . On this basis, K I is a measure of the severity of the crack. Its definition in a
            formal mathematical sense is
                                                       √

                                          K I = lim  σ y 2πr                           (8.8)
                                               r,θ→0
               It is generally convenient to express K I as
                                                     √
                                             K I = FS πa                               (8.9)
            where the factor F is needed to account for different geometries. For example, if a central crack
            in a plate is relatively long, Eq. 8.2 needs to be modified, as the proximity of the specimen edge
            causes F to increase above unity. The quantity F is a function of the ratio a/b, as shown in Fig. 8.12,
            curve (a). Curves (b) and (c) show the variation of F with a/b for two additional cases of cracked
            members under tension, specifically, for double-edge-cracked plates and for single-edge-cracked
            plates.

            8.3.3 Additional Comments on K and G

            For loading in Mode II or III, analogous, but distinct, stress field equations exist, and stress
            intensities K II and K III can be defined in a manner analogous to K I . However, most practical
            applications involve Mode I. As a convenience, the subscript on K I will be dropped, and K without
            such a subscript is understood to denote K I , that is, K = K I .
               The quantities G and K can be shown to be related as follows:
                                                    K  2
                                                G =                                   (8.10)
                                                     E

            where E is obtained from the material’s elastic modulus E and Poisson’s ratio ν:
                                    E = E         (plane stress; σ z = 0)

                                          E                                           (8.11)

                                    E =           (plane strain; ε z = 0)
                                        1 − ν 2
            Equation 8.10 and the dependence of G on load versus displacement behavior, Eq. 8.6, can be
            exploited to evaluate K. Slopes on P-v curves, as in Fig. 8.9, are employed in a procedure called
            the compliance method. See any book on fracture mechanics or Tada (2000) for details.
               Since G and K are directly related according to Eq. 8.10, only one of these concepts is
            generally needed. We will primarily employ K, which is consistent with most engineering-oriented
            publications on fracture mechanics.


            8.4 APPLICATION OF K TO DESIGN AND ANALYSIS

            For fracture mechanics to be put to practical use, values of stress intensity K must be determined
            for crack geometries that may exist in structural components. Extensive analysis work has been
            published, and also collected into handbooks, giving equations or plotted curves that enable K
            values to be calculated for a wide variety of cases. A special section of the References at the
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