Update
I've underestimated Taylor expansions. They actually work. I assumed that integral of the remainder term can be unbounded, but with a little work it can be shown that this is not the case.
The Taylor expansion works for functions in bounded closed interval. For random variables with finite variance Chebyshev inequality gives
$$P(|X-EX|>c)\le \frac{\operatorname{Var}(X)}{c}$$
So for any $\varepsilon>0$ we can find large enough $c$ so that
$$P(X\in [EX-c,EX+c])=P(|X-EX|\le c)<1-\varepsilon$$
First let us estimate $Ef(X)$. We have
\begin{align}
Ef(X)=\int_{|x-EX|\le c}f(x)dF(x)+\int_{|x-EX|>c}f(x)dF(x)
\end{align}
where $F(x)$ is the distribution function for $X$.
Since the domain of the first integral is interval $[EX-c,EX+c]$ which is bounded closed interval we can apply Taylor expansion:
\begin{align}
f(x)=f(EX)+f'(EX)(x-EX)+\frac{f''(EX)}{2}(x-EX)^2+\frac{f'''(\alpha)}{3!}(x-EX)^3
\end{align}
where $\alpha\in [EX-c,EX+c]$, and the equality holds for all $x\in[EX-c,EX+c]$. I took only $4$ terms in the Taylor expansion, but in general we can take as many as we like, as long as function $f$ is smooth enough.
Substituting this formula to the previous one we get
\begin{align}
Ef(X)&=\int_{|x-EX|\le c}f(EX)+f'(EX)(x-EX)+\frac{f''(EX)}{2}(x-EX)^2dF(x)\\\\
&+\int_{|x-EX|\le c}\frac{f'''(\alpha)}{3!}(x-EX)^3dF(x)
+\int_{|x-EX|>c}f(x)dF(x)
\end{align}
Now we can increase the domain of the integration to get the following formula
\begin{align}
Ef(X)&=f(EX)+\frac{f''(EX)}{2}E(X-EX)^2+R_3\\\\
\end{align}
where
\begin{align}
R_3&=\frac{f'''(\alpha)}{3!}E(X-EX)^3+\\\\
&+\int_{|x-EX|>c}\left(f(EX)+f'(EX)(x-EX)+\frac{f''(EX)}{2}(x-EX)^2+f(X)\right)dF(x)
\end{align}
Now under some moment conditions we can show that the second term of this remainder term is as large as $P(|X-EX|>c)$ which is small. Unfortunately the first term remains and so the quality of the approximation depends on $E(X-EX)^3$ and the behaviour of third derivative of $f$ in bounded intervals. Such approximation should work best for random variables with $E(X-EX)^3=0$.
Now for the variance we can use Taylor approximation for $f(x)$, subtract the formula for $Ef(x)$ and square the difference. Then
$E(f(x)-Ef(x))^2=(f'(EX))^2\operatorname{Var}(X)+T_3$
where $T_3$ involves moments $E(X-EX)^k$ for $k=4,5,6$. We can arrive at this formula also by using only first-order Taylor expansion, i.e. using only the first and second derivatives. The error term would be similar.
Other way is to expand $f^2(x)$:
\begin{align}
f^2(x)&=f^2(EX)+2f(EX)f'(EX)(x-EX)\\\\
&+[(f'(EX))^2+f(EX)f''(EX)](X-EX)^2+\frac{(f^2(\beta))'''}{3!}(X-EX)^3
\end{align}
Similarly we get then
\begin{align*}
Ef^2(x)=f^2(EX)+[(f'(EX))^2+f(EX)f''(EX)]\operatorname{Var}(X)+\tilde{R}_3
\end{align*}
where $\tilde{R}_3$ is similar to $R_3$.
The formula for variance then becomes
\begin{align}
\operatorname{Var}(f(X))=[f'(EX)]^2\operatorname{Var}(X)-\frac{[f''(EX)]^2}{4}\operatorname{Var}^2(X)+\tilde{T}_3
\end{align}
where $\tilde{T}_3$ have only third moments and above.