Page 360 - T. Anderson-Fracture Mechanics - Fundamentals and Applns.-CRC (2005)
P. 360

1656_C007.fm  Page 340  Monday, May 23, 2005  5:54 PM





                       340                                 Fracture Mechanics: Fundamentals and Applications
























                       FIGURE 7.39  Fracture toughness master curve. Taken from E 1921-03, ‘‘Standard Test Method for Deter-
                       mination of Reference Temperature, T o , for Ferritic Steels in the Transition Range.’’ American Society for
                       Testing and Materials, Philadelphia, PA, 2003.


                          According to the master curve model, the temperature dependence of median toughness in the
                       ductile-brittle transition region is given by

                                               K       =   + 30  70  exp[ .019 ( −  T  T  )]     (7.32)
                                                                  0
                                                Jc(median  )                o
                       where T  is a reference transition temperature in °C and the units of K  are  MPa m  . At T = T ,
                             o
                                                                                                     o
                                                                                Jc
                       the median fracture toughness = 100  MPa m . Once T  is known for a given material, the fracture
                                                                   o
                       toughness distribution can be inferred as a function of temperature through Equation (7.28) and
                       Equation (7.32).
                          The first step in determining T  is to perform replicate fracture toughness tests at a constant
                                                   o
                       temperature. ASTM E 1921 recommends at least six such tests. Next, the data are converted to
                       equivalent 1T values using Equation (7.29).  These data are then put into Equation (7.30) to
                       determine K  at the test temperature. The median toughness at this temperature is computed from
                                o
                       Equation (7.31). Finally, T  is computed by rearranging Equation (7.32):
                                            o
                                                T  T =  −    1    ln   K  Jc(median  )  − 30    (7.33)
                                                o
                                                        0 019.      70   
                       ASTM E 1921 provides an alternative method for determining T  when K  data are obtained at
                                                                                    Jc
                                                                            o
                       multiple temperatures.
                          Figure 7.39 schematically illustrates the fracture toughness master curve for a particular steel.
                       By combining Equation (7.28) and Equation (7.32), it is possible to infer median, upper-bound and
                       lower-bound toughness as a function of temperature.
                          The Master Curve approach works best in the ductile-brittle transition region. It may not fit
                       data in the lower shelf very well, and it is totally unsuitable for the upper shelf. Equation (7.32)
                       increases without bound with increasing temperature, and thus does not model the upper shelf.


                       7.9 QUALITATIVE TOUGHNESS TESTS

                       Before the development of formal fracture mechanics methodology, engineers realized the impor-
                       tance of material toughness in avoiding brittle fracture. In 1901, a French scientist named G. Charpy
                       developed a pendulum test that measured the energy of separation in notched metallic specimens.
                       This energy was believed to be indicative of the resistance of the material to brittle fracture.
   355   356   357   358   359   360   361   362   363   364   365