Alternate approach.
For statement (I), substitute $w=1/z$ so the behaviour near $z=0$ becomes the behaviour of $g(w)=\sin(1/\cos w)$ as $w\to\infty$. The function $\cos w$ has infinitely many zeros $w=\frac{\pi}{2}+k\pi$, $k\in\mathbb{Z}$, spread across the whole $w$-plane, and each gives a point where $g$ has an essential singularity. Translating back through $z=1/w$, these correspond to points $z_k=\frac{2}{(2k+1)\pi}$ that pile up at $z=0$ as $|k|\to\infty$. A singularity is isolated only if some punctured disk around it contains no other singular point; here every punctured disk about $0$, however small, contains infinitely many $z_k$. So $z=0$ fails the isolation test and statement (I) is false.
For statement (II), use the standard Laurent (cosecant) expansion valid for $0<|z|<\pi$:
\[\csc z=\frac{1}{z}+\frac{z}{6}+\frac{7z^3}{360}+\cdots\]
Then
\[\frac{1}{z\sin z}=\frac{1}{z}\csc z=\frac{1}{z}\left(\frac{1}{z}+\frac{z}{6}+\frac{7z^3}{360}+\cdots\right)=\frac{1}{z^2}+\frac{1}{6}+\frac{7z^2}{360}+\cdots\]
There is no $z^{-1}$ term, so the residue at the only enclosed singularity $z=0$ is $0$, and by Cauchy's residue theorem
\[\oint_{|z|=1}\frac{dz}{z\sin z}=2\pi i(0)=0.\]
This confirms statement (II) is true while (I) is false, so the correct choice is only (II).
\[\boxed{\text{Only (II)}}\]