Another way to proceed is to transform variables to spherical coordinates.
To that end, let $x=r \sin \theta \cos \phi$, $y=r\sin \theta \sin \phi$, and $z=r\cos \theta$, where $0\le \theta \le \pi$ and $0\le \phi \le 2\pi$. Then, the limit that is in question is
$$\lim_{r\to 0}\left(\frac{\sin r^2}{r(|\sin \theta \cos \phi|+|\sin \theta \sin \phi|+|\cos \theta|)}\right)=0$$
To see this, note that
$$\lim_{r\to 0} \frac{\sin r^2}{r} =0,$$
which can be shown using L'Hospital's Rule. It is important to note that for all $0\le \theta \le \pi$ and $0\le \phi \le 2\pi$, $1\le|\sin \theta \cos \phi|+|\sin \theta \sin \phi|+|\cos \theta| \le \sqrt{3}$ is bounded.
Now, for the entire problem, we need to examine the limit
$$\lim_{r\to 0} \left(\frac{\sin r^2+\tan (r(\sin \theta \cos \phi +\sin \theta \sin \phi + \cos \theta))}{r(|\sin \theta \cos \phi|+|\sin \theta \sin \phi|+|\cos \theta|)}\right)$$
Clearly, the limit as $r \to 0$ does not exist inasmuch as its value depends on the values of $\theta$ and $\phi$. For example, if $\theta =0$, then the limit is $1$ since $\sin \theta \cos \phi +\sin \theta \sin \phi + \cos \theta = 1$, $|\sin \theta \cos \phi|+|\sin \theta \cos \phi|+|\cos \theta| =1$ and
$$\lim_{r\to 0} \frac{\sin r^2}{r} =0$$
$$\lim_{r\to 0} \frac{\tan r}{r} = 1$$
which can be easily shown by using L'Hospital's Rule. This first limit is, in fact, the limit that was in question.
If $\theta = \pi$, then the limit is $-1$ since $\sin \theta \cos \phi +\sin \theta \sin \phi + \cos \theta = -1$, $|\sin \theta \cos \phi|+|\sin \theta \cos \phi|+|\cos \theta| =1$ and
$$\lim_{r\to 0} \frac{\sin r^2}{r} =0$$
$$\lim_{r\to 0} \frac{\tan (-r)}{r} = -1$$
Inasmuch as the limit is non-unique, it does not exist.