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48 2. Introductory applications



          In this  section, we  will  describe a  technique (for  equations which  contain a small
          parameter,  as in those  above) which is  a  natural  extension of simply  obtaining an
          asymptotic expansion of a function, examining its breakdown, rescaling, and so on.
            We will begin by examining the simple  quadratic equation




          and seek the solutions for  The essential idea is to obtain different asymptotic
          approximations for    valid for different sizes of x, and see if these  admit  (ap-
          proximate) roots. Given that        we  could have  roots anywhere on  the
          real line, and so all sizes of x must be examined. (We will consider, first, only the real
          roots of equations; the  extension to  complex roots  will be  discussed in due course.)
          One further comment is required at this stage: we describe here a technique for find-
          ing roots  that builds on  the ideas  of singular perturbation  theory. In  practice,  other
          approaches are likely to be used in conjunction with ours to solve particular equations
          e.g.  sketching or plotting the function, or using a standard numerical procedure  (such
          as Newton-Raphson). There is no suggestion that this expansion technique should be
          used in isolation—it is simply one  of a number of tools available.
            Returning to (2.1), if x = O(1), then




          and  so  we have a  root x = – 1  (approximately).  In  order  to  generate  a better ap-
          proximation, we may use any appropriate method. For example, we could invoke the
          familiar procedure of iteration,  so we may write




          with        Then we obtain




          and so on (but note that iteration may not generate a correct asymptotic expansion at
          a given order in   It is clear from this approach that a complete representation of the
          root will be  obtained if we use  the asymptotic sequence   and so an alternative is
          to seek this form directly—and this is more in keeping with the ideas of perturbation
          theory. Thus we might seek a root in the form





          so that (2.1) can be written as
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