Page 78 - Schaum's Outline of Differential Equations
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CHAP. 7]           APPLICATIONS  OF FIRST-ORDER  DIFFERENTIAL  EQUATIONS               61



               which has as its solution


               At t= 0, we are given that v = 0. Substituting these  values into  (_/), we  obtain


               from  which we conclude  that c = -16  and  (_/)  becomes



                                                                              2
               (a)  From  (_/)  or  (2),  we  see  that as  t  —> °°, v  —>  16  so  the  limiting velocity  is  16  ft/sec .
               (b)  To find  the time it takes  for the ball to hit the ground (x = 3000), we need  an expression  for the position  of the
                   ball  at any time t. Since  v = dx/dt,  (2) can  be rewritten as





                   Integrating both  sides of this last equation  directly with respect  to t, we  have


                   where c 1 denotes  a constant  of integration. At  t = 0, x = 0. Substituting these  values into (3), we obtain



                   from  which we conclude  that  Cj = -8  and (3)  becomes




                   The  ball hits the ground  when x(t) = 3000.  Substituting this value into (4), we have



                   or
                   Although (5) cannot  be solved explicitly for t, we can approximate  the solution by trial and error, substituting
                   different  values  of  t into  (5) until  we  locate  a  solution  to the  degree  of  accuracy  we  need.  Alternatively, we
                   note  that  for  any  large value of  t, the  negative  exponential  term will be negligible. A  good  approximation  is
                   obtained  by setting 2t = 376  or t = 188 sec.  For this value of  t, the exponential  is essentially  zero.

         7.13.  A body  weighing 64 Ib is dropped from  a height of  100 ft with  an initial  velocity  of  10 ft/sec.  Assume
               that  the air resistance is proportional to the velocity of the body.  If the limiting velocity is known  to be
               128 ft/sec, find  (a) an expression for the velocity of the body  at any time t and  (b) an expression for  the
               position of the body at any time t.
               (a)  Locate the coordinate  system  as in Fig.  7-5.  Here  w = 64  Ib.  Since  w = mg,  it follows that mg = 64, or m = 2
                   slugs. Given that v : = 128 ft/sec, it follows from  (7.6)  that 128 = 641k, or  k = j. Substituting these values into
                   (6.4),  we obtain  the linear differential  equation




                   which has the solution


                   At  t = 0, we are given that v =  10. Substituting these values into (_/), we have  10 = ce° + 128,  or c = -118. The
                   velocity at any time t is given by
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