According to Bohr's model, the energy of the electron in the \( n \)-th orbit is given by:
\[
E_n = - \frac{13.6 \, \text{eV}}{n^2}
\]
We are given the energy \( E = -3.4 \, \text{eV} \). To find \( n \), we solve for \( n \) in the equation:
\[
-3.4 = - \frac{13.6}{n^2}
\]
\[
n^2 = \frac{13.6}{3.4} = 4
\]
\[
n = 2
\]
Thus, the electron is in the second energy level (\( n = 2 \)).
The angular momentum \( L \) of the electron in the \( n \)-th orbit is given by:
\[
L = n \hbar
\]
where \( \hbar = \frac{h}{2\pi} \) is the reduced Planck’s constant.
For \( n = 2 \):
\[
L = 2 \hbar
\]
Thus, the angular momentum of the electron is:
\[
\boxed{L = 2 \hbar}
\]