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178  4. The method of multiple scales



                               we obtain






            Before we proceed with the details, we should make an important observation. The
          transform, (4.61), defining the fast scale  (usually called the phase in these problems),
          implies a consistency condition that must exist if  is a twice-differentiable function,
          namely





          this additional  equation is  called the conservation of waves (or  of wave  crests), and  it
          arises quite naturally from an elementary argument. Consider (one-dimensional) waves
          entering and leaving the  region   the number of waves, per unit time,  crossing
            into the region is given as   and the number leaving, across x, we will write as
          The total number of waves (wave crests) between   and x is   if the number of
          waves does not change (which is what is typically observed, even if they change shape)
          then





          or, upon allowing differentiation with respect to x,




          which immediately recovers (4.63) if the dependence on  (x, t) is via (X, T).
            Returning to equation (4.62), we seek a solution






          with


          and then we obtain the sequence of equations
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