Note that Solovay-Kitaev theorem holds for unitaries on qu$d$it (section 5 in DN05), then we can set $d=2^n$ for $n$-qubit unitary. Following the same analysis, we obtain
- length of gate sequences $l_{\epsilon} = O(\ln^{\ln 5/\ln(3/2)} (1/\epsilon))$,
- time complexity $t_{\epsilon} = O(\ln^{\ln 3/\ln(3/2)}(1/\epsilon))$.
Now the issue is the accuracy parameter $\epsilon$. Since $SU(d)$ is $(d^2-1)$-dimension manifold, so to approximate every gate in $SU(d)$ within $\epsilon_0$, we generate $O(1/\epsilon_0^{d^2-1})$ sequences.
Hence, for any specific universal gate set $\mathcal{G}$ the length of gate sequences $$l_0 \geq O\left(\frac{d^2-1}{\log |\mathcal{G}|} \log(1/\epsilon_0)\right).$$
Set $d=2^n$ for $n$ qubits, then we obtain $l_0 \sim 4^n \mathrm{poly}\log(1/\epsilon)$. Therefore, you indeed need exponentially many gates for approximating unitaries on $n$ qubits.