Phase angle \( \phi = \tan^{-1} \left( \frac{\omega L}{R} \right) \)
Given: \( f = 350 \, \text{Hz}, L = 0.1 \, \text{H}, R = 110 \, \Omega \)
\[
\omega = 2\pi f = 2\pi \cdot 350 \approx 2200 \Rightarrow \frac{\omega L}{R} = \frac{2200 \cdot 0.1}{110} = 2
\]
So, \( \phi = \tan^{-1}(2) \)