This problem links two separate ideas from the Bohr model, the energy of a hydrogen orbit and its angular momentum, so it's solved in two stages: first pin down which orbit the electron is in, then apply the angular momentum rule to that orbit.
Finding the orbit number: In the Bohr model, the energy of the \( n \)-th orbit of hydrogen is \( E_n = -\dfrac{13.6}{n^2}\,\text{eV} \). Setting this equal to the given energy:
\[ -3.4 = -\frac{13.6}{n^2} \quad \Rightarrow \quad n^2 = \frac{13.6}{3.4} = 4 \quad \Rightarrow \quad n = 2 \]So the electron sits in the second orbit.
Applying the angular momentum rule: Bohr's quantization condition states that angular momentum in the \( n \)-th orbit can only take the values:
\[ L = \frac{nh}{2\pi} \]Substituting \( n = 2 \):
\[ L = \frac{2h}{2\pi} = \frac{h}{\pi} \]This is a direct, single-formula substitution once the orbit number is known, no further steps are needed since angular momentum in the Bohr model depends only on \( n \).
Therefore, the angular momentum of the electron in this orbit is \( \dfrac{h}{\pi} \).