Page 174 - Schaum's Outline of Differential Equations
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CHAPTER        18







                                              Graphical and




            Numerical                                Methods for




                           Solving                        First-Order




              Differential Equations












         QUALITATIVE METHODS

            In Chapter 2, we touched upon the concept  of qualitative methods  regarding differential equations; that is,
         techniques  which  are  used  when  analytical  solutions  are  difficult  or  virtually impossible  to  obtain.  In  this
         chapter,  and  in  the  two  succeeding  chapters,  we  introduce  several  qualitative  approaches  in  dealing  with
         differential  equations.


         DIRECTION   FIELDS

            Graphical methods produce plots of solutions to first-order differential equations  of the form



         where the derivative appears only on the left  side of the  equation.

                                                                                       1
         Example 18.1.  (a) For the problem / = -y  + x + 2, we have/(jt, y) = -y + x + 2. (b) For the problem / = y  + 1, we have
                2
         f(x,  y) = y  + 1.  (c)  For  the  problem  y' = 3,  we  have (x,  y)  = 3.  Observe  that  in  a  particular  problem, (x,  y)  may  be
                                                f
                                                                                      f
         independent of x, of y, or of x and y.
            Equation  (18.1) defines the slope of the solution curve y(x) at any point  (x, y) in  the plane. A line element
         is a short line segment that begins at the point (x, y) and has a slope specified by (18.1); it represents an approxi-
         mation to the solution curve through that point. A collection  of line elements is a direction field. The graphs of
         solutions to (18.1) are generated  from  direction fields  by drawing curves that pass through the points at which
         line elements are drawn and also are tangent to those line elements.
            If  the  left  side  of  Eq.  (18.1)  is  set  equal  to  a  constant,  the  graph  of  the  resulting  equation  is  called  an
         isocline. Different  constants define different  isoclines, and each isocline has the property that all line  elements

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