For the first-order linear ordinary differential equation, an integrating factor is
Multiplication converts the left side to a derivative:
Integrating gives . The initial value fixes , so
On a branch with , the given derivative is nonzero wherever the original equation is defined, so use inverse-function linearization of a first-order equation and regard as a function of :
The integrating factor gives
Thus the nonzero solutions are given implicitly by
Each branch must also retain ; at those excluded points the original right-hand side is undefined and the inverse graph cannot represent a regular . Differentiating the implicit equation gives , equal to the required quotient wherever these restrictions hold.
The additional solution , on any interval avoiding , was lost when dividing by and must be included. It is not defined through the point in the original equation.
For , the Bernoulli differential equation becomes linear under . Multiplying the equation by gives
On an interval with , the integrating factor is , hence
Therefore the complete set of solution branches is
The original equation requires ; each nonzero branch additionally requires . The zero solution is restored explicitly because the reciprocal substitution excludes it.

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