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51. (a) For computing torques, we choose the axis to be at support 2 and consider torques which encourage
        counterclockwise rotation to be positive. Let m = mass of gymnast and M = mass of beam. Thus,
        equilibrium of torques leads to

                                  M g(1.96 m) − mg(0.54 m) − F1 (3.92 m) = 0 .

        Therefore, the upward force at support 1 is F1 = 1163 N (quoting more figures than are significant
        – but with an eye toward using this result in the remaining calculation).
    (b) Balancing forces in the vertical direction, we have

                                             F1 + F2 − M g − mg = 0

        so that the upward force at support 2 is F2 = 1.74 × 103 N.

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P13 051

  • 1. 51. (a) For computing torques, we choose the axis to be at support 2 and consider torques which encourage counterclockwise rotation to be positive. Let m = mass of gymnast and M = mass of beam. Thus, equilibrium of torques leads to M g(1.96 m) − mg(0.54 m) − F1 (3.92 m) = 0 . Therefore, the upward force at support 1 is F1 = 1163 N (quoting more figures than are significant – but with an eye toward using this result in the remaining calculation). (b) Balancing forces in the vertical direction, we have F1 + F2 − M g − mg = 0 so that the upward force at support 2 is F2 = 1.74 × 103 N.