For the Bernoulli differential equation, work on a branch where and the required powers are defined. Multiplication by makes the chain rule useful:
Thus , and . The case is already linear and must be treated separately, because the proposed substitution would be constant. Solutions lost by dividing by a power of , particularly when it solves the original equation, must also be checked separately.
Here , so obeys . An integrating factor is , giving
The nonzero solutions are therefore
The additional solution is . Each formula is interpreted on an interval where is defined and its displayed denominator is nonzero.
The given particular solution suggests the standard reduction of a Riccati equation. Substitution of gives
On either side of , an integrating factor is , so . Hence
along with the separately recovered particular solution . The denominator must remain nonzero on the solution interval; is a singular point of the divided differential equation.
For the positive- branch, and . Nonsingular endpoint values exclude , so
The particular solution gives the same value directly. These evaluations concern one solution branch, with a common integration constant, rather than independently chosen solutions at the two points.

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