Page 184 - Schaum's Outline of Theory and Problems of Applied Physics
P. 184

CHAP. 14]                        SIMPLE HARMONIC MOTION                               169



        SOLVED PROBLEM 14.5
              An object of unknown mass is suspended from a spring, which stretches by 10 cm as a result. If the
              system is set in oscillation, what will its frequency be?
                  The force F that causes the spring to stretch by s = 10 cm = 0.1 m is the weight mg of the unknown mass, so
              the force constant of the spring is
                                                F    mg
                                             k =  =      = 10mg m −1
                                                s   0.1m
              The period of oscillation of the system is therefore



                                     m           m                1
                              T = 2π    = 2π          = 2π                = 0.635 s
                                                                        2
                                                                −1
                                      k      10mg m −1      (10 m )(9.8 m/s )
              and the frequency is f = 1/T = 1.58 Hz.
        SOLVED PROBLEM 14.6
              A spring whose force constant is 12 lb/ft oscillates up and down with a period of 0.5 s when a wrench is
              suspended from it. How much does the wrench weigh?
                  Since m = w/g,


                                             m       w
                                      T = 2π   = 2π
                                              k      gk
                                                      2
                                          gkT  2  (32 ft/s )(12 lb/ft)(0.5s) 2
                                     w =      =                     = 2.4lb
                                          4π  2         4π  2
        DISPLACEMENT,VELOCITY, AND ACCELERATION
        If t = 0 when a body undergoing simple harmonic motion is in its equilibrium position of s = 0 and is moving
        in the direction of increasing s, then at any time t thereafter its displacement is
                                               s = A sin 2πft

        Often this formula is written

                                                s = A sin ωt
        where ω = 2πf is the angular frequency of the motion in radians per second. (If instead the body is at s =+A
        when t = 0, then s = A cos 2πft = A cos ωt.) Figure 14-2 is a graph of s versus t.



















                                                 Fig. 14-2
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