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22  1. Mathematical preliminaries



            Thus we  have two  representations of  one valid for x = O(1),  (1.44), and
          one for       (1.47). Further, the latter expansion is defined on X = 0 (i.e. x = 0)
          and gives the  correct value  (as an expansion  of   With  these observations in
          place, we are now in a position to discuss uniformity and breakdown more completely
          and more carefully.


          1.6 UNIFORMITY OR BREAKDOWN
          Suppose that we wish to represent  for     by  an asymptotic expansion





          which has been constructed for x = O(1). This expansion is uniformly valid if




          for every    and       Conversely,  it breaks down (and is therefore non-uniform)
          if there is some  and  some      such that



          In other words, the  expansion  is  said to  break  down if there is  a  size of x, in  the
          domain of the function, for which two consecutive terms in the asymptotic expansion
          are the same size. On the other hand, the expansion is uniformly valid if the asymptotic
          ordering of the terms, as represented by the asymptotic sequence  is  maintained
          for all x in the domain.
            It is an elementary exercise to apply this principle to our previous example;  from
          (1.44) we have




          and the domain of the original function is  As   the  second  term in the
          expansion, (1.48), becomes the same size as the first where  the expansion
          has broken down.  That is,  for x of this size, the expansion  (1.48) is no longer valid;
          in order to determine the form of the expansion for  we must return to the
          function and use this choice i.e.  write    is  exactly how we generated
          (1.47). Thus  the  breakdown of an  expansion can  lead us to  the  choice of a  new,
          scaled variable, and we note that this is based on the properties of the expansion, not
          any additional  or  special  knowledge  about the  underlying function.  (This  point is
          important for what will come later: when we solve differential equations, we will not
          have the exact solution available—only an asymptotic expansion of the solution. But,
          as we shall see, the equation itself does hold information about possible scalings.) We
          apply this principle of breakdown and rescaling to another example.
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