Page 137 - Schaum's Outline of Differential Equations
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120                   SECOND-ORDER  LINEAR DIFFERENTIAL  EQUATIONS               [CHAP.  14




         14.4.  Determine  the  circular  frequency,  natural  frequency,  and  period  for  the  simple  harmonic  motion
               described  in Problem  14.1.
               Circular  frequency:
               Natural  frequency:
               Period:

         14.5.  A  10-kg mass is attached  to a spring, stretching it 0.7 m from  its natural length. The mass is started in
               motion  from  the equilibrium  position  with an initial  velocity of  1 ml sec in the upward direction.  Find
               the subsequent motion, if the force due to air resistance is -90i N.
                                 2
                  Taking g = 9.8 m/sec , we have w = mg = 98 N and k = w/l = 140 N/m. Furthermore, a = 90 and F(t) = 0 (there
               is no external  force). Equation  (14.1)  becomes


               The roots of the associated  characteristic  equation  are Xj = -2  and ^ = -7,  which are real and distinct; hence this
               problem is an example  of overdamped motion. The  solution of  (1) is


               The initial conditions are x(0)  = 0 (the mass  starts at the equilibrium position) and i(0) = -1 (the initial velocity is
                                                                                        2
                                                                                    7
               in the negative direction). Applying these conditions, we find that c 1 = — c 2 = --|, so that x = ^(e" '  -  e~ ').  Note that
               x  —> 0 as  t  —>  °°; thus, the  motion  is transient.

         14.6.  A mass of 1/4 slug is attached to a spring, whereupon the spring is stretched  1.28 ft from its natural length.
               The mass is started in motion from the equilibrium position with an initial velocity of 4 ft/sec in the down-
               ward direction.  Find the subsequent motion of the mass if the force due to air resistance is  -2ilb.
                  Here  m=l/4,  a = 2,  F(t) = Q  (there  is  no  external  force),  and,  from  Hooke's  law, k = mgll
               = (l/4)(32)/1.28 = 6.25. Equation  (14.1)  becomes



               The roots of the associated  characteristic equation are Xj = -4  + O and ^ = -4 -  13, which are complex conjugates;
               hence  this problem is an example  of oscillatory damped  motion. The  solution of (1) is


               The  initial  conditions  are x(0) = 0 and i(0) = 4. Applying these  conditions,  we find  that  Cj = 0 and  c 2 = |; thus,
                    4
               x = |e~ ' sin3t. Since x  —> 0 as  t  —> m, the motion is transient.

         14.7.  A mass of 1/4 slug is attached to a spring having a spring constant of 1 Ib/ft. The mass is started in motion
               by initially displacing it 2 ft in the downward direction  and giving it an initial velocity of 2 ft/sec  in the
               upward direction. Find the subsequent motion of the mass, if the force due to air resistance is -lilb.
                  Here m = 1/4, a = 1, k =1, and F(t)  = 0. Equation  (14.1)  becomes


               The roots of the associated  characteristic equation are  A^ =  A^ = -2,  which are equal; hence this problem is an  example
               of critically damped  motion. The  solution of  (1) is


               The initial  conditions  are x(0)  = 2 and i(0) = -2  (the initial  velocity is in the negative direction). Applying these
               conditions, we find  that Cj = c 2 = 2. Thus,



               Since x  —> 0 as  t  —>  °°, the  motion  is transient.
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