In mathematics, an Abel equation of the first kind, named after Niels Henrik Abel, is any ordinary differential equation that is cubic in the unknown function. In other words, it is an equation of the form

${\displaystyle y'=f_{3}(x)y^{3}+f_{2}(x)y^{2}+f_{1}(x)y+f_{0}(x)\,}$

where ${\displaystyle f_{3}(x)\neq 0}$. If ${\displaystyle f_{3}(x)=0}$ and ${\displaystyle f_{0}(x)=0}$, or ${\displaystyle f_{2}(x)=0}$ and ${\displaystyle f_{0}(x)=0}$, the equation reduces to a Bernoulli equation, while if ${\displaystyle f_{3}(x)=0}$ the equation reduces to a Riccati equation.

The substitution ${\displaystyle y={\dfrac {1}{u}}}$ brings the Abel equation of the first kind to the "Abel equation of the second kind" of the form

${\displaystyle uu'=-f_{0}(x)u^{3}-f_{1}(x)u^{2}-f_{2}(x)u-f_{3}(x).\,}$

The substitution

${\displaystyle {\begin{aligned}\xi &=\int f_{3}(x)E^{2}~dx,\\[6pt]u&=\left(y+{\dfrac {f_{2}(x)}{3f_{3}(x)}}\right)E^{-1},\\[6pt]E&=\exp \left(\int \left(f_{1}(x)-{\frac {f_{2}^{2}(x)}{3f_{3}(x)}}\right)~dx\right)\end{aligned}}}$

brings the Abel equation of the first kind to the canonical form

${\displaystyle u'=u^{3}+\phi (\xi ).\,}$

Dimitrios E. Panayotounakos and Theodoros I. Zarmpoutis discovered an analytic method to solve the above equation in an implicit form.^[1]