Page 36 - Marks Calculation for Machine Design
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P1: Shibu
                          January 4, 2005
                 Brown˙C01
        Brown.cls
                  18
                            U.S. Customary 12:26  STRENGTH OF MACHINES  SI/Metric
                  Example 2. Determine the shear stress (τ i )  Example 2. Determine the shear stress (τ i )
                  at the inside surface of a hollow circular shaft,  at the inside surface of a hollow circular shaft,
                  where                              where
                     T = 8,000 ft · lb = 96,000 in · lb  T = 12,000 N · m
                    D o = 4in = 2R o                   D o = 10 cm = 0.1 m = 2R o
                    D i = 2in = 2R i                   D i = 5cm = 0.05 m = 2R i
                  solution                           solution
                  Step 1. Calculate the polar moment of inertia  Step 1. Calculate the polar moment of inertia
                  (J) of the shaft using Eq. (1.23).  (J) of the shaft using Eq. (1.23).
                            1     4  4                      1     4  4
                         J =  π R − R i                  J =  π R − R i
                                                                 o
                                 0
                            2                               2
                            1      4     4                  1        4        4
                          =  π((2in) − (1in) )            =   π((0.05 m) − (0.025 m) )
                            2                               2
                          = 23.56 in 4                    = 0.00000920 m 4
                  Step 2. Substitute this value for (J), the torque  Step 2. Substitute this value for (J), the torque
                  (T ), and the inside radius (R i ) into Eq. (1.21).  (T ), and the inside radius (R i ) in Eq. (1.21).
                          TR i  (96,000 in · lb)(1in)      TR i  (12,000 N · m)(0.025 m)
                      τ i =  =                         τ i =  =
                           J       23.56 in 4               J      0.00000920 m 4
                                                                      2
                                 2
                        = 4,074 lb/in = 4.1 kpsi         = 32,600,000 N/m = 32.6MPa
                  Level of Torque Reduction.  For the geometry of Example 2, the outside radius (R o )
                  is twice the inside radius (R i ). It is interesting that reduction in torque carrying capa-
                  bility of the hollow shaft compared to the solid shaft is small. This is because the
                  material near the center of the shaft carries very little of the shear stress, or load, pro-
                  duced by the applied torque (T ). It is instructive to determine the exact value of this
                  reduction.
                    Start with the fact that the maximum shear stress (τ max ) will be the same for both the
                  shafts, because they are made of the same material and the outside radius (R o ) is the same.
                  This fact is shown mathematically in Eq. (1.21) to both the solid shaft and the hollow shaft.
                  This fact is shown mathematically in Eq. (1.24) as


                                           T solid R o  T hollow R o
                                                 =                             (1.24)
                                            J solid  J hollow

                    The outside radius (R o ) cancels on both sides, so Eq. (1.24) can be rearranged to give
                  the ratio of the torque carried by the hollow shaft (T hollow ) divided by the torque carried by
                  the solid shaft (T solid ).


                                            T hollow  J hollow
                                                  =                            (1.25)
                                             T solid  J solid
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