The Burger's vortex in 2 Dimension - solving Differential equation After simplifying the vortex equation, I get to this equation:

$$
-\alpha y \partial_y \omega = \alpha \omega + \nu \partial_{yy} \omega
$$

where the $\alpha$ and $\nu$ are constant values and $\omega(y)$. I want to solve the equation for $\omega(y)$. How can I do it? I appreciate in advance for kind helps.

Regards,

Ehsan
$$
-\alpha y \dfrac{d\omega}{dy} = \alpha\omega + \nu \dfrac{d^2\omega}{dy^2}
$$

this is the same as

$$
\nu \dfrac{d^2\omega}{dy^2} + \alpha \dfrac{d}{dy}(y\omega) = 0
$$
thus

$$
\nu \omega ' + \alpha y \omega + C = 0
$$

now if $C=0$ then the solution is separable but if not then we have to solve
$$
\frac{d\omega}{dy} + \frac{\alpha}{\nu} y \omega= -C
$$
using integrating factor
$$
\omega \mathrm{e}^{\frac{\alpha}{\nu}\frac{y^2}{2}} = -\int_0^y C \mathrm{e}^{\frac{\alpha}{\nu}\frac{y'^2}{2}}dy'
$$

or

$$
\omega(y) = -\left(\int_0^y C \mathrm{e}^{\frac{\alpha}{\nu}\frac{y'^2}{2}}dy'\right)\mathrm{e}^{-\frac{\alpha}{\nu}\frac{y^2}{2}}
$$
Maple finds solutions
$$ \omega(y) = \left(c_1 + c_2\; \text{erfi}\left(\sqrt{-\alpha/(2\nu)} y\right)\right) e^{-\alpha y^2/(2 \nu)}$$