This is a solution using the direct method of Lyapunov. (using other procedures might be more straightforward here)
The system is nonautonomous (time variant), therefore, a time variant Lyapunov function might be suited for the problem.
Consider the Lyapunov function:
$V = a(t)\frac{1}{2}x_1^2 + b(t)\frac{1}{2}x_2^2$,
where $0<a(t)<a_1$, $\forall t$ and $0<b(t)<b_1$, $\forall t$, with constants $a_1,\,b_1$. The parameters $a(t)$ and $b(t)$ must be determined. ($a$ and $b$ must be positive and bounded that $V$ is positive definite.)
The derivative along the trajectories of the system
$\dot x_1 = x_2 - \frac{x_1 \cos{t}}{k_0 + \sin{t}}
\\
\dot x_2 = - x_2 - x_1(k_0 + \sin{t}) , k_0 > 1$
is:
\begin{align}
\dot V & = \dot a \frac{1}{2}x_1^2 + a x_1 \dot x_1 + \dot b \frac{1}{2}x_2^2 + b x_2 \dot x_2 \\
& = \dot a \frac{1}{2}x_1^2+ \dot b \frac{1}{2}x_2^2\\
& \quad+ a x_1 ( x_2 - \frac{x_1 \cos{t}}{k_0 + \sin{t}}) \\
& \quad+ bx_2(- x_2 - x_1(k_0 + \sin{t}) )\\
& = \dot a \frac{1}{2}x_1^2+ \dot b \frac{1}{2}x_2^2\\
& \quad + a x_1 x_2 - a x_1^2\frac{ \cos{t}}{k_0 + \sin{t}} \\
& \quad - b x_2^2 - x_1x_2 b (k_0 + \sin{t}) ) \\
&= -( a\frac{ \cos{t}}{k_0 + \sin{t}} -\dot a \frac{1}{2})x_1^2 - (b-\dot b \frac{1}{2})x_2^2 \\
& \quad+ (a-b(k_0 + \sin{t}) ))x_1x_2
\end{align}
Now choose $b =\sin(t) + k_0 >0$ and $a = (\sin(t) + k_0)^2>0$, i.e. $\dot a = 2\cos(t)(\sin(t) + k_0) $, $\dot b = \cos(t)$:
\begin{align}
\dot V & \leq - (\sin(t) + k_0 - \frac{\cos(t)}{2})x_2^2 \leq 0, \quad \text{for} \,\,k_0>\sqrt{5}/2\approx 1.1
\end{align}
The derivative of $V$ is negative semi definite, i.e., the origin is stable.
Since the system is time varying, the standard invariance principle can not be considered to investigate asymptotic stability. Then, usually Barbalat's Lemma is considered. Roughly it says that: If a function $\phi(t)$, with $\lim_{t\to\infty} \phi(t)= c<\infty$, has a uniformly continuous derivative, then $\lim_{t\to \infty}\dot \phi(t) \to 0$. For the problem here, we can say that $V$ is lower bounded, $\dot V$ is negative semidefinite, (hence we know that V converges to a limit) and it is uniformly continuous since
$\ddot V = - (\sin(t) + k_0 - \frac{\cos(t)}{2})x_2(- x_2 - x_1(k_0 + \sin{t})) - (\cos(t) + k_0 - \frac{\sin(t)}{2})x_2^2 $
is bounded. (This can be concluded since $x_1$ and $x_2$ converge to finite limits.)
Hence, $\dot V \to 0$ for $t \to \infty$. For $x_2 \equiv 0$, $x_1$ must also be zero as it can be obtained from the system equations.
The origin is even exponentially stable.
In summary:
$V = \frac{(\sin(t) + k_0)^2}{2}x_1^2 + \frac{(\sin(t) + k_0)}{2}x_2^2$, positive definite and decrescent
$\dot V \leq - (\sin(t) + k_0 - \frac{\cos(t)}{2})x_2^2 \leq 0$, for $k_0>\sqrt{5}/2$,
negative semi definit $\Rightarrow$ Lyapunov stable equilibrium
Barbalat's Lemma can be applied $\Rightarrow$ asymptotically stable equilibrium