Page 40 - Schaum's Outline of Differential Equations
P. 40

CHAP.  4]            SEPARABLE  FIRST-ORDER  DIFFERENTIAL  EQUATIONS                  23



                        2 3
         4.2.  Solve / = y- * .
                  We first  rewrite this equation  in the differential  form (see Chapter  3) jr  dx -  (lly  ) dy  = 0. Then A(x)  = jr and
                       2
               B(y)  = -lly .  Substituting these  values into Eq. (4.2), we have


                                                4
               or, by performing the indicated  integrations, x /4  + lly  = c. Solving explicitly for y,  we obtain  the solution as






         4.3.  Solve

                  This equation  may be rewritten in the differential form
                                               2
                                              (x +2)dx-ydy  = 0
                                      2
               which is separable  with A(x)  =x  + 2 and B(y)  = -y.  Its solution is



               or


               Solving for y, we obtain  the solution in implicit form as




               with k = -2c. Solving for y implicitly, we obtain  the two solutions


                                                   and



         4.4.  Solve / = 5y.
                  First rewrite this equation  in the differential form 5 dx— (lly)  dy = 0, which is separable.  Its solution is



               or, bv evaluating, 5x  — In  lyl  =  c.
                  To solve  for y explicitly, we  first  rewrite  the  solution  as  In  md  then  take the  exponential  of  both
               sides. Thus,      Noting that     we obtain                  The  solution is given explicitly
               byy  =
                  Note  that  the  presence  of  the  term  (—lly)  in  the  differential  form  of  the  differential  equation  requires  the
                                                                                                5x
               restriction y ^ 0 in our derivation of the solution. This restriction is equivalent to the restriction k ^ 0, since y = ke .
                                                                                      Sx
               However,  by inspection, y = 0 is a solution of the differential  equation  as originally given. Thus, y = ke  is the solution
               for  all k.
                  The differential equation as originally given is also linear. See Problem  6.9 for an alternate  method  of solution.

         4.5.  Solve

                  This equation,  in differential form, is(x = 1) dx + (-y4 - 1) dy =0.  which is  separable.  Its solution is
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