To solve this problem, we need to analyze the behavior of a series LCR (Inductor-Capacitor-Resistor) circuit when components are removed one at a time.
Initially, when the inductor \( L \) is removed, the circuit becomes an RC (Resistor-Capacitor) circuit. In an RC circuit, the phase difference (\( \phi \)) between current and voltage is given by:
\(\phi = \tan^{-1} \left( \frac{-1}{\omega RC} \right)\)
It is given that the phase difference is \( \frac{\pi}{3} \), so:
\(\phi = -\frac{\pi}{3}\)
When the capacitor \( C \) is removed, the circuit becomes an RL (Resistor-Inductor) circuit. In an RL circuit, the phase difference is given by:
\(\phi = \tan^{-1} \left( \frac{\omega L}{R} \right)\)
Again, it is given that the phase difference is \( \frac{\pi}{3} \), so:
\(\phi = \frac{\pi}{3}\)
The key insight is that the same phase difference \( \frac{\pi}{3} \) is obtained regardless of whether \( L \) or \( C \) is removed. This symmetry indicates that the circuit is at resonance when all components are present. At resonance in an LCR circuit:
\(\omega L = \frac{1}{\omega C}\)
At resonance, the phase difference between voltage and current is 0, which implies current and voltage are in phase. Therefore, the power factor \( \text{cos} \phi \) is \( 1 \).
Thus, the power factor of the circuit when all components are present is 1.
Therefore, the correct answer is 1.