Consider the following ODE: $y'+ y = \epsilon y^2, y(0,\epsilon)=1$
Assuming the perturbation amsats gives:
$y'_0 + y_0 =0, y_0(0)=1,$
$y'_1 + y_1 = y^2_0$, $y_1(0)=0$
How is: $y_0(x)=e^{(-x)}$ and $y_1(x) = e^{(-x)}-e^{(-2x)}$
Consider the following ODE: $y'+ y = \epsilon y^2, y(0,\epsilon)=1$
Assuming the perturbation amsats gives:
$y'_0 + y_0 =0, y_0(0)=1,$
$y'_1 + y_1 = y^2_0$, $y_1(0)=0$
How is: $y_0(x)=e^{(-x)}$ and $y_1(x) = e^{(-x)}-e^{(-2x)}$
Here you can, to confirm the perturbartion computations, solve the problem directly as a Bernoulli equation to find that $$ \frac{d}{dx}(y^{-1})=-y^{-2}y'=-ϵ+y^{-1}\implies y^{-1}(x)=ϵ+(1-ϵ)e^{x} $$ and then $$ y(x)=\frac{e^{-x}}{1-ϵ(1-e^{-x})} $$ which you can expand as geometric series to find the perturbation series.