Because the original differential equation divides by , its domain requires and . Set , so . The equation becomes the first-order linear differential equation
An integrating factor is , since . Thus
Returning to gives the explicit general real solutions
Each sign is fixed on a connected interval where and the radicand is strictly positive. The strict condition excludes , where the original differential equation is undefined. There is no additional zero solution.
Where , divide by it to obtain . The integrating factor is , and the product rule gives
The initial condition gives . Hence
The simplified expression has a differentiable extension through , with . Direct substitution verifies the original undivided differential equation there as well: its left side is . Thus the maximal interval containing on which this solution is finite is ; the apparent exclusion of arose only from division by . This is continuation through a zero of the leading ODE coefficient.

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