If $$\frac{\tan (\alpha + \beta - \gamma )}{\tan (\alpha - \beta + \gamma )}=\frac{\tan \gamma}{\tan \beta}$$ then prove $$\sin (\beta - \gamma)=0$$ or $$\sin 2\alpha + \sin2\beta + \sin 2\gamma =0$$ here my try goes -
To prove $\sin (\beta - \gamma)=0$, sin x = 0, only when x = 0 or 360 degree, but for the sake of simplicity let's take x = 0, then we've to prove that $\beta - \gamma =0$ or $\beta = \gamma$.
Now,
If $\beta = \alpha$, then first equation will be $\frac{\tan \alpha}{\tan \alpha}= \frac{\tan\gamma}{\tan\beta}$ or $\frac{\tan\gamma}{\tan\beta}=1$
and
$$\frac{\tan x}{\tan y}=1$$, only if $$\tan x = \tan y$$
So, also in this case $\tan \gamma$ must be equal to $\tan \beta$ so, as to prove that $\sin (\beta - \gamma)=0$.
So, how to prove that $\beta = \gamma$?
and how to solve the second part of the question here?
Let's define $\mu := \frac12(\beta+\gamma)$ and $\nu:=\frac12(\beta-\gamma)$, so that we have $$\frac{\tan(\alpha+2\nu)}{\tan(\alpha-2\nu)} = \frac{\tan(\mu-\nu)}{\tan(\mu+\nu)} \quad\to\quad \frac{\sin(\alpha+2\nu)\cos(\alpha-2\nu)}{\sin(\alpha-2\nu)\cos(\alpha+2\nu)}=\frac{\sin(\mu-\nu)\cos(\mu+\nu)}{\sin(\mu+\nu)\cos(\mu-\nu)}$$ The identity $$\sin(p\pm q)\cos(p \mp q) = \sin p \cos p \pm \sin q \cos q = \frac12( \sin 2p \pm \sin 2q) \tag{$\star$}$$ gives us $$\frac{\sin 2\alpha + \sin 4\nu}{\sin 2\alpha - \sin 4 \nu} = \frac{\sin 2\mu - \sin 2 \nu }{\sin 2 \mu + \sin 2\nu}$$ so that, upon cross-multiplying and combining terms, $$\begin{align} 0 &= \sin 2\alpha \cdot 2 \sin 2\nu + \sin 4\nu \cdot 2\sin 2\mu \\ &= \sin 2\alpha \cdot 2 \sin 2\nu + 2\sin 2\nu \cos 2\nu \cdot 2\sin 2\mu \\ &= 2\sin 2\nu\left(\; \sin 2\alpha + 2\sin2\mu\cos 2\nu \;\right) \\ &= 2\sin(\beta-\gamma)\left(\; \sin 2\alpha + 2\sin(\beta+\gamma)\cos(\beta-\gamma) \;\right) \\ &= 2\sin(\beta-\gamma)\left(\; \sin 2\alpha + \sin 2 \beta + \sin 2\gamma \;\right) \qquad\text{(using $(\star)$ again)} \\ \end{align}$$
Therefore, $$\sin(\beta-\gamma) = 0 \qquad\text{or}\qquad \sin 2\alpha + \sin 2 \beta + \sin 2\gamma = 0$$ $\square$