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28. (a) Computing torques about the hinge, we find the tension in the wire:

                                                                           Wx
                                      T L sin θ − W x = 0 =⇒ T =                  .
                                                                          L sin θ

    (b) The horizontal component of the tension is T cos θ, so equilibrium of horizontal forces requires that
        the horizontal component of the hinge force is

                                                  Wx                   Wx
                                         Fx =               cos θ =           .
                                                 L sin θ              L tan θ

    (c) The vertical component of the tension is T sin θ, so equilibrium of vertical forces requires that the
        vertical component of the hinge force is

                                                   Wx                         x
                                     Fy = W −               sin θ = W 1 −             .
                                                  L sin θ                     L

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P13 028

  • 1. 28. (a) Computing torques about the hinge, we find the tension in the wire: Wx T L sin θ − W x = 0 =⇒ T = . L sin θ (b) The horizontal component of the tension is T cos θ, so equilibrium of horizontal forces requires that the horizontal component of the hinge force is Wx Wx Fx = cos θ = . L sin θ L tan θ (c) The vertical component of the tension is T sin θ, so equilibrium of vertical forces requires that the vertical component of the hinge force is Wx x Fy = W − sin θ = W 1 − . L sin θ L