Page 34 - Marks Calculation for Machine Design
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P1: Shibu
                          January 4, 2005
                                      12:26
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                 Brown˙C01
                                           STRENGTH OF MACHINES
                  16
                  and substituting the force (F) for the shear force (V ), area (A) for a round hole from
                  Eq. (1.17), the ultimate shear strength (S su ) can be expressed by Eq. (1.19).
                                                    F
                                              S su =                           (1.19)
                                                   2πrt
                    Solving for the required punching force (F) in Eq. (1.19) gives Eq. (1.20).
                                             F = S su (2πrt)                   (1.20)
                            U.S. Customary                       SI/Metric
                  Example 3. Calculate the required punching  Example 3. Calculate the required punching
                  force (F) for round hole, where    force (F) for round hole, where
                    S su = 35,000 psi (aluminum)       S su = 240 MPa (aluminum)
                     r = 0.375 in                       r = 1cm = 0.01 m
                      t = 0.25 in                       t = 0.65 cm = 0.0065 m
                  solution                           solution
                  Step 1. Calculate the required punching force  Step 1. Calculate the required punching force
                  (F) from Eq. (1.20).               (F) from Eq. (1.20).
                    F = S su (2πrt)                    F = S su (2πrt)
                      = (35,000 psi)(2π(0.375 in)(0.25 in))  = (240 MPa)(2π(0.01 m)(0.0065 m))
                                     2
                                                                         2
                      = (35,000 psi)(0.589 in )         = (240 MPa)(0.00041 m )
                      = 20,620 lb = 20.6 kip            = 98,020 N = 98.0kN



                  1.4 TORSION


                  Figure 1.19 shows a circular shaft acted upon by opposing torques (T ), causing the shaft
                  to be in torsion. This type of loading produces a shear stress in the shaft, thereby causing
                  one end of the shaft to twist about the axis relative to the other end.


                                            T            T




                                        FIGURE 1.19  Torsion.


                  Stress. The two opposing torques (T ) produce a twisting load along the axis of the shaft,
                  resulting in a shear stress distribution (τ) as given by Eq. (1.21),

                                              Tr
                                          τ =       0 ≤ r ≤ R                  (1.21)
                                              J
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