7. In a series RL circuit, under what circumstances would \( \phi \) be \( 0^{\circ} \) or \( 90^{\circ} \) ? ( \( \phi \) will be zero if the circuit is purely resistive) ( \( \phi \) will be \( 90^{\circ} \) if the circuit is purely inductive). 8. In a series RC circuit, under what circumstances would \( \phi \) be exactly \( 0^{\circ} \) or \( -90^{\circ} \) ? ( \( \phi \) will be zero if the circuit is purely resistive) ( \( \phi \) will be \( -90^{\circ} \) if the circuit is purely capacitive).
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The Deep Dive
In a series RL circuit, the phase angle \( \phi \) describes the relationship between voltage and current. If you have a purely resistive circuit, where the resistance is the only component in play, the current and voltage are perfectly in sync, resulting in \( \phi = 0^{\circ} \). Conversely, in a purely inductive circuit, the inductor creates a scenario where the current lags the voltage by a quarter cycle, giving you that cool \( \phi = 90^{\circ} \) vibe! On the flip side, in a series RC circuit, things get thrilling! When the circuit is all about resistance, and no capacitance is influencing the game, the phase angle continues to sit pretty at \( 0^{\circ} \)—current and voltage dance together beautifully! But once you switch to a purely capacitive scene, where the capacitor dominates, the current leads the voltage, causing a phase angle of \( -90^{\circ} \). Looks like resistance and capacitance have their own unique styles!