I like $\dot x$ etc. better than $x'$ etc., so I'll use the "dot" notation for time derivatives. This being said, the given equations become
$\dot x = xe^{y - 3} \tag{1}$
and
$\dot y = 2\sin x + 3 - y. \tag{2}$
At an equilibrium point, we have $\dot x = \dot y = 0$, so
$xe^{y - 3} = 0 \tag{3}$
and
$2\sin x + 3 - y = 0. \tag{4}$
Since $e^{y - 3} \ne 0$ for all $y \in \Bbb R$, (3) yields $x = 0$; then by (4), $y = 3$; there are no other equilibria. $(x, y) = (3, k\pi)$, $k \in \Bbb Z$, is not an equilibrium as direct substitution of these values into (1)-(4) will reveal.
The Jacobian $J(x, y)$ of the system (1)-(2) at the point $(x, y)$ is given by the matrix
$J(x, y) = \begin{bmatrix} \dfrac{\partial {\dot x}}{\partial x} & \dfrac{\partial {\dot x}}{\partial y} \\ \dfrac{\partial {\dot y}}{\partial x} & \dfrac{\partial {\dot y}}{\partial y} \end{bmatrix} = \begin{bmatrix} e^{y - 3} & xe^{y - 3} \\ 2\cos x & -1 \end{bmatrix}; \tag{5}$
at $(0, 3)$ we have
$J(0, 3) = \begin{bmatrix} 1 & 0 \\ 2 & -1 \end{bmatrix}. \tag{6}$
It is easy to see that the characteristic polynomial of the matrix $J(0, 3)$ is $\lambda^2 -1$; the eigenvalues are thus $\pm 1$, as may also easily be seen by inspection of the triangular matrix $J(0, 3)$. Since $J(0, 3)$ has one positive and one negative eigenvalue, the point $(0, 3)$ is a saddle; hence, it is an unstable equilibrium.
Hope this helps. Cheers,
and as always,
Fiat Lux!!!