Page 303 - Marks Calculation for Machine Design
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P1: Shashi
                          January 4, 2005
                                      15:4
        Brown.cls
                 Brown˙C07
                              U.S. Customary  FATIGUE AND DYNAMIC DESIGN  SI/Metric  285
                    Step 5. Using Eq. (6.23), along with the given  Step 5. Using Eq. (6.23), along with the given
                    values for the geometric stress concentration  values for the geometric stress concentration
                    factor (K t ) and notch sensitivity (q), calculate  factor (K t ) and notch sensitivity (q), calculate
                    the reduced stress concentration factor (K f ) as  the reduced stress concentration factor (K f ) as
                     K f = 1 + q(K t − 1) = 1 + (0.8)(2.15 − 1)  K f = 1 + q(K t − 1) = 1 + (0.8)(2.15 − 1)
                       = 1 + 0.92 = 1.92                  = 1 + 0.92 = 1.92
                    Step 6. Using the reduced stress concentration  Step 6. Using the reduced stress concentration
                    factor (K f ) found in step 5, calculate the mis-  factor (K f ) found in step 5, calculate the mis-
                    cellaneous effects factor (k e ) using Eq. (7.16)  cellaneous effects factor (k e ) using Eq. (7.16)
                    as                                 as
                              1    1                             1    1
                          k e =  =    = 0.52                 k e =  =    = 0.52
                              K f  1.92                          K f  1.92
                    Step 7. Using the given ultimate tensile stress  Step 7. Using the given ultimate tensile stress
                    (S ut ) and Eq. (7.1), calculate the test specimen  (S ut ) and Eq. (7.1), calculate the test specimen
                    endurance limit (S ) as            endurance limit (S ) as


                                e                                 e


                       S = 0.504 S ut = (0.504)(120 kpsi)  S = 0.504 S ut = (0.504)(840 MPa)
                        e
                                                          e
                         = 60.5 kpsi                       = 423.4MPa
                    Step 8. Using the test specimen endurance  Step 8. Using the test specimen endurance

                    limit (S ) found in step 7 and the modifying  limit (S ) found in step 7 and the modifying

                         e                                  e
                    factors found in steps 1 through 6, calculate the  factors found in steps 1 through 6, calculate the
                    endurance limit (S e ) for the machine element  endurance limit (S e ) for the machine element
                    using the Marin equation in Eq. (7.7) as  using the Marin equation in Eq. (7.7) as
                     S e = k a k b k c k d k e S       S e = k a k b k c k d k e S
                                  e                                 e
                       = (0.76)(0.87)(1)(1)(0.52)(60.5 kpsi)  = (0.76)(0.87)(1)(1)(0.52)(423.4MPa)
                       = (0.344)(60.5 kpsi) = 20.8 kpsi  = (0.344)(423.4MPa) = 145.6MPa
                      Notice that the biggest reduction, almost 50 percent, in the endurance limit (S e ) for the
                    machine element came from the stress concentration caused by the transverse hole in the
                    shaft. Accounting for all five factors reduced the endurance limit (S e ) to one-third the test

                    specimen endurance limit (S ) found from the R. R. Moore rotating-beam machine. This
                                         e
                    translates into a minimum factor-of-safety (n = 3) to have a safe design under repeated
                    reversed loading. Again, this is why the first law of machine design is “When in doubt,
                    make it stout!”
                      Consider now the possibility that the dynamic loading is fluctuating rather than being
                    completely reversed as has been the assumption so far.
                    7.4 FLUCTUATING LOADING


                    The second type of dynamic loading to be presented is called fluctuating loading, where
                    the load on the machine element varies about some mean stress (σ m ), which can be
                    positive or negative, by an amount called the alternating stress (σ a ). Note that if the
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