Page 304 - Schaum's Outline of Differential Equations
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CHAP. 28]           SERIES  SOLUTIONS NEAR A REGULAR  SINGULAR POINT                 287



                                       2
                                                   3
         28.21.  Find  the indicial equation  of x y"  + xe*y'  + (x  -  \)y = 0 if the solution is required  near x = 0.
                  Here



               and we have





                                                                                     2
               from  which/7 0 = 1 and q Q = —1. Using (_/) of Problem  28.20, we obtain the indicial equation as X  -  1 = 0.

         28.22.  Solve Problem  28.9 by an alternative method.
                                           2
                  The  given differential  equation, 3x y"  — xy'  + y = 0, is a special  case of Ruler's  equation


               where bj(j=0,  1, ...  , n)  is a constant. Euler's equation can always be transformed into a linear differential  equation
               with constant  coefficients  by the change  of variables



               It follows from  (2) and  from  the chain rule and  the product rule of differentiation  that












                  Substituting Eqs. (2), (3),  and  (4) into the given differential  equation and  simplifying,  we obtain





               Using the method of Chapter  9 we find  that the solution of this last equation is y = c^ + c 2e <1/3)z . Then using (2)
                                 1 113
               and noting that e (1/3)z  = (e ) ,  we have as before,



         28.23.  Solve the differential  equation  given in Problem  28.12 by an alternative method.
                                          2
                  The  given differential  equation, x y"  — xy'  + y = 0, is a special  case of Euler's equation,  (_/)  of Problem  28.22.
               Using the transformations (2), (3), and  (4) of Problem  28.22, we reduce the given equation to




                                                           z
               The solution to this equation is (see Chapter 9) y = c^ + c 2ze . Then, using (2) of Problem 28.22, we have for the
               solution of the original differential  equation


               as before.
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