Page 145 - Schaum's Outline of Theory and Problems of Applied Physics
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130                                   EQUILIBRIUM                                [CHAP. 11



        SOLVED PROBLEM 11.2
              A 500-kg load is suspended from the end of a horizontal boom, as in Fig. 11-2(a). The angle between the
              boom and the cable supporting its end is 45 . Assuming that the boom’s mass can be neglected compared
                                                ◦
              with that of the load, find (a) the tension in the cable and (b) the inward force the boom exerts on the wall.





















                                                    Fig. 11-2



              (a) The three forces that act on the end of the boom are the weight w of the load, the tension T in the cable, and
                  the outward force F exerted by the boom. A free-body diagram of these forces is shown in Fig. 11-2(b). The x
                  and y components of these forces have the magnitudes
                                                             ◦
                                        T x =−T cos θ =−T cos 45 =−0.707T
                                        T y = T sin θ = T sin 45 = 0.707T
                                                          ◦
                                                                2
                                        w =−mg =−(500 kg)(9.8 m/s ) =−4900 N
                                         F = ?
                  The condition for translational equilibrium in the y (vertical) direction yields

                                              F y = T y + w = 0
                                           0.707T − 4900 N = 0
                                                           4900 N
                                                       T =       = 6930 N
                                                           0.707
              (b) To find the inward force the boom exerts on the wall, we start with the condition for equilibrium in the x
                  (horizontal) direction:
                                      F x = T x + F = 0

                                      −0.707T + F = 0
                                               F = 0.707T = (0.707)(6930 N) = 4900 N

                  The inward force on the wall must have the same magnitude as the outward force on the load; hence, the inward
                  force is also equal to 4900 N.

        SOLVED PROBLEM 11.3

              A 50-lb box is suspended by a rope from the ceiling. If a horizontal force of 20 lb is applied to the box,
              what angle will the rope make with the vertical?
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