\begin{align} \tan \frac \alpha 2 & = u \\[4pt] \alpha & = 2\arctan u \\[4pt] d\alpha & = \frac{2\,du}{1+u^2} \\[4pt] \sin\alpha & = \sin(2\arctan u) = 2(\sin\arctan u) (\cos \arctan u) \\[4pt] & = 2\,\frac u {\sqrt{1+u^2}} \cdot \frac 1 {\sqrt{1+u^2}} = \frac{2u}{1+u^2} \end{align} $$ \frac{\hspace{6cm}}{} \qquad \S \qquad \frac{\hspace{6cm}}{} $$
The well known substitution above is for the moment my preferred approach to solving the differential equation $$ \frac{d\alpha}{\sin\alpha} = \frac{d\beta}{\sin\beta}. \tag{differential equation} $$ One gets $$ \frac{d\alpha}{\sin\alpha} = \frac{\left( \dfrac{2\,du}{1+u^2} \right)}{\left( \dfrac{2u}{1+u^2} \right)} = \frac{du} u $$ and writing $v = \tan \dfrac\beta 2$, we then have $$ \frac{du} u = \frac {dv} v $$ so that $\log u = \log v + \text{constant}$ and so $u = v\times \text{constant}$, and finally $$ \tan \frac\alpha 2 = \text{constant} \times \tan \frac\beta 2. \tag{solution} $$ So my question is whether there are other ways to approach this that are either better or otherwise worth some attention.