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Chapter 1 of 12 • Page 1 of 248🔒 Protected PDF • Watermarked
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ElectricalBasic Electrical
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In pure inductor circuit, average power is

A

0

B

1

C

∞\infty∞

D

1.414

Correct Answer

Concept & PrincipleElectricalBasic Electrical
Option A

0

Quick Summary: In a pure inductive circuit, the average power dissipated over one complete cycle is zero. This occurs because the inductor stores energy in its magnetic field during one quarter of a cycle and returns that exact same energy to the source in the next quarter cycle.

💡 Explanation

In a pure inductive circuit, the average power dissipated over one complete cycle is zero. This occurs because the inductor stores energy in its magnetic field during one quarter of a cycle and returns that exact same energy to the source in the next quarter cycle.

🔢 Key Formulas

Pavg=VrmsIrmscos⁡(ϕ)P_{avg} = V_{rms} I_{rms} \cos(\phi)Pavg​=Vrms​Irms​cos(ϕ) — General average power formula

ϕ=90°\phi = 90°ϕ=90° — Phase angle for a pure inductor

⚙️ Working Principle

In an AC circuit with a pure inductor, the voltage VVV leads the current III by a phase angle of 90°90°90° (π/2{\pi/2}π/2 radians). The average power is calculated using the formula Pavg=VrmsIrmscos⁡(ϕ)P_{avg} = V_{rms} I_{rms} \cos(\phi)Pavg​=Vrms​Irms​cos(ϕ), where ϕ\phiϕ is the phase difference. Since ϕ=90°\phi = 90°ϕ=90°, cos⁡(90°)=0\cos(90°) = 0cos(90°)=0, leading to zero net power consumption.

📌 Key Points
  • ▸

    A pure inductor is a lossless component.

  • ▸

    Power factor (cosϕcos \phicosϕ) for a pure inductor is 0 (lagging).

  • ▸

    Energy is only stored in the magnetic field, not dissipated as heat.

  • ▸

    The net work done over a full cycle is zero.

✅ Advantages
  • ▸

    Does not consume real power (no energy wastage).

  • ▸

    Used effectively in reactive power compensation.

❌ Disadvantages / Limitations
  • ▸

    Cannot be used for heating or lighting purposes.

  • ▸

    Causes voltage drops in transmission lines due to inductive reactance.

🛠️ Applications / Uses
  • ▸

    Induction motors (for magnetic field creation).

  • ▸

    Tuned circuits and filters.

  • ▸

    Smoothing reactors in power supplies.

📄 Additional Information
  • ▸

    Option B (1) represents a purely resistive circuit where phase angle is 0.

  • ▸

    Option C (infinity) is physically impossible for passive components.

  • ▸

    Option D (1.414) represents the peak factor for a sinusoidal waveform (sqrt2\\sqrt{2}sqrt2).

📊 Diagram / Illustration
Average Power Formula
Pavg=VrmsIrmscos⁡(ϕ)P_{avg} = V_{rms} I_{rms} \cos(\phi)Pavg​=Vrms​Irms​cos(ϕ)
For Pure Inductor: ϕ=90∘\phi = 90^\circϕ=90∘
cos⁡(90∘)=0  ⟹  Pavg=0\cos(90^\circ) = 0 \implies P_{avg} = 0cos(90∘)=0⟹Pavg​=0
✅

A is correct — The average power in a pure inductor is zero because it does not dissipate energy as heat, acting only as an energy storage element.

Core Concepts Used
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Inductive Reactance ($X_L$) Phase Angle ($phi$) Power Factor ($cos \phi$) Reactive Power
💡 EXAM TIP

Remember: Resistors dissipate real power (P=I2RP = I^2RP=I2R), whereas Inductors and Capacitors only exchange reactive power with the source.

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