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220 5. Some worked examples arising from physical problems



            We introduce





          and then the equation for            becomes



          We seek a solution, periodic in T and bounded in   in the familiar form





          and so obtain






          and so on. The initial conditions give







          The general solution for   from (5.61a), is




          for arbitrary functions  and  the  initial conditions, (5.62a,c), require that




          and so we select




            Equation (5.61b) then becomes




          where                is periodic in T, i.e. in   only if
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