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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