Step 1: For element \( X \), voltage and current are in phase, which means that the impedance is purely resistive. Therefore, \( X \) must be a resistor.
Step 2: For element \( Y \), \( V \) leads \( I \) by \( \frac{\pi}{4} \). This suggests that element \( Y \) behaves like an inductor, because in an inductor, the current lags the voltage, and at high frequencies, the phase difference between voltage and current increases, but here we are given that voltage leads current, which is a characteristic of inductive reactance at a specific frequency.
Step 3: For element \( Z \), \( I \) leads \( V \) by \( \frac{\pi}{4} \), which indicates capacitive behavior, because in a capacitor, current leads voltage by \( \frac{\pi}{2} \) at high frequencies, and at lower frequencies, this phase difference decreases.
Conclusion:
- \( X \) is a resistor,
- \( Y \) is an inductor,
- \( Z \) is a capacitor.