Write , so . The chain rule givesHence and the Cauchy-Euler equation becomesIts characteristic equation is . The distinct roots give . Returning to the original independent variable givesThe same form holds on any negative interval avoiding , using ; the stated substitution covers the positive interval. At the differential equation is singular, so crossing it is a separate extension problem.
Seek a particular solution . Substitution into the linear ordinary differential equation gives , so . Add the complementary solution from part (a):The two prescribed values yield and . Thus , so and . ThereforeDirect substitution gives and , and the homogeneous solution contributes zero to the left-hand differential operator.
On an interval avoiding , divide by to obtain the first-order linear ordinary differential equationAn integrating factor is . Multiplying through and using the product rule givesBy integration by parts, . ConsequentlyThe formula differentiates back to the original equation. Although division excluded , this formula has a smooth extension there with , satisfying the original equation at zero as well.
The substitution gives . Cancelling on both sides of the differential equation, for , givesThe initial condition is . This selects a positive solution locally, so separation of variables givesUsing gives , and continuity selects the positive square root:The real solution containing has maximal positive domain . Its denominator tends to zero and as , a finite-time blow-up of an ordinary differential equation in the independent variable . Thus the source's wording “for ” needs this domain restriction; the prescribed initial value admits no real solution on the whole positive half-line. The division by loses the separate solution , but that solution does not meet the initial condition.
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