For , multiply by to obtain the first-order linear ordinary differential equation . Its integrating factor is . The product rule then gives
Integration yields , so
The constant of integration is arbitrary on each connected interval of the original equation's domain. The formula extends smoothly through zero, but the printed equation itself contains and is not defined there.
The real equation has domain . Its integrating factor is
Thus the linear ordinary differential equation becomes . After integration, . The initial condition gives , hence

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