Page 135 - Marks Calculation for Machine Design
P. 135

P1: Sanjay
                          January 4, 2005
                 Brown˙C02
        Brown.cls
                           V
                             0        16:18      BEAMS                       x    117
                                                                        L
                                                              –
                           –wL
                           FIGURE 2.108  Shear force diagram.


                      Note that the shear force (V ) is zero at the left end of the beam and decreases linearly to
                    a negative value (−wL) at the right end of the beam. This shear force distribution is given
                    by Eq. (2.73).

                                                 V =−wx                         (2.73)

                      Therefore, the maximum shear force (V max ) is given by Eq. (2.74).

                                                V max = wL                      (2.74)

                      The bending moment distribution is given by Eq. (2.75) for all values of the distance (x)
                    equal to zero at the left end of the beam to a value (L) at the right end of the beam. (Always
                    measure the distance (x) from the left end of any beam.)

                                                wx 2
                                          M =−        0 ≤ x ≤ L                 (2.75)
                                                 2
                      The bending moment (M) distribution is shown in Fig. 2.109.


                           M

                              0                                               x
                                                                          L
                                                                   –
                             2
                          –wL /2
                          FIGURE 2.109  Bending moment diagram.


                      The bending moment (M) is zero at the left end of the beam and then decreases quadrat-
                                                   2
                    ically to a maximum negative value (−wL /2) at the right end. The maximum bending
                    moment (M max ) occurs at the right end of the beam as given by Eq. (2.76).

                                                      wL 2
                                               M max =                          (2.76)
                                                       2
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