Tangent's derivatives are not cyclic. If you differentiate $e^x$, $\cos(x)$, $\sin(x)$ and even $\sinh(x)$ and $\cosh(x)$ enough times, you'll eventually end up with the original function providing a nice formula for the Taylor coefficients. A way to state this periodicity is to say that they all satisfy a differential equation of the form $y^{(n)}=y$ for some $n$. This property means that their Taylor Series will have some kind of periodic relation among the coefficients.
Not so with tangent.
Instead, tangent satisfies the differential equation $y'=1+y^2$. This is because $\frac{d}{dx}\tan(x) = \sec^2(x) = 1+\tan^2(x)$, via the Pythagorean Theorem. This can be used to compute specific values for the coefficients. But the general form of the Taylor Expansion is
$$
\tan(x) = \sum_{n=1}^{\infty}\frac{(-1)^{n-1}2^{2n}(2^{2n}-1)B_{2n}}{2n(2n-1)!}x^{2n-1}
$$
where the $B_n$ are the Bernoulli Numbers, which are defined to be the Taylor Series coefficients of $\frac{x}{e^x-1}$. I'll let ProofWiki provide the proof of this formula.