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Chapter 1 of 12 • Page 1 of 248🔒 Protected PDF • Watermarked
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ElectricalBasic Electrical
PrevNext

Which is true for series resonance?

A

Z=RZ = RZ=R

B

XL=XCX_L = X_CXL​=XC​

C

I=VRI = \frac{V}{R}I=RV​

D

All of above

Correct Answer

Concept & PrincipleElectricalBasic Electrical
Option D

All of above

Quick Summary: In an RLC series circuit, resonance occurs when the inductive reactance equals the capacitive reactance, causing them to cancel each other out. This results in the circuit behaving as a purely resistive load, where impedance is minimum and current is maximum.

💡 Explanation

In an RLC series circuit, resonance occurs when the inductive reactance equals the capacitive reactance, causing them to cancel each other out. This results in the circuit behaving as a purely resistive load, where impedance is minimum and current is maximum.

🔢 Key Formulas

XL=2πfrLX_L = 2\pi f_r LXL​=2πfr​L — Inductive Reactance

XC=12πfrCX_C = \frac{1}{2\pi f_r C}XC​=2πfr​C1​ — Capacitive Reactance

Z=R2+(XL−XC)2Z = \sqrt{R^2 + (X_L - X_C)^2}Z=R2+(XL​−XC​)2​ — Total Impedance

fr=12πLCf_r = \frac{1}{2\pi\sqrt{LC}}fr​=2πLC​1​ — Resonant Frequency

⚙️ Working Principle

The inductive reactance XL=2πfLX_L = 2\pi fLXL​=2πfL increases with frequency, while capacitive reactance XC=12πfCX_C = \frac{1}{2\pi fC}XC​=2πfC1​ decreases. At the resonant frequency frf_rfr​, these magnitudes equalize (XL=XCX_L = X_CXL​=XC​), nullifying the imaginary part of the impedance Z=R+j(XL−XC)Z = R + j(X_L - X_C)Z=R+j(XL​−XC​). Consequently, the total impedance ZZZ simplifies to the resistance RRR, and the circuit power factor becomes unity.

📌 Key Points
  • ▸

    At resonance, the phase angle between voltage and current is zero.

  • ▸

    The circuit provides minimum impedance to the source at the resonant frequency.

  • ▸

    Voltage magnification occurs across the inductor and capacitor.

  • ▸

    The circuit acts as a band-pass filter configuration.

✅ Advantages
  • ▸

    Maximum current flow for a given voltage source

  • ▸

    Selectivity in radio tuning circuits

❌ Disadvantages / Limitations
  • ▸

    Risk of voltage breakdown due to high Q-factor

  • ▸

    Sensitive to frequency variations

🛠️ Applications / Uses
  • ▸

    Radio frequency tuning circuits

  • ▸

    Band-pass filter designs

  • ▸

    Induction heating systems

📄 Additional Information
  • ▸

    The Q-factor (Quality Factor) determines the sharpness of the resonance curve: Q=1RLCQ = \frac{1}{R}\sqrt{\frac{L}{C}}Q=R1​CL​​.

  • ▸

    If XL>XCX_L > X_CXL​>XC​, the circuit is inductive (lagging pf); if XC>XLX_C > X_LXC​>XL​, it is capacitive (leading pf).

📊 Diagram / Illustration
Series Resonance ConditionsXₗ = X꜀Z = RI = VR
✅

D is correct — All listed conditions (Z=RZ=RZ=R, XL=XCX_L=X_CXL​=XC​, I=V/RI=V/RI=V/R) define the state of resonance in an RLC series circuit.

Core Concepts Used
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Resonance Impedance Complex Reactance
💡 EXAM TIP

Always remember that resonance in series circuits leads to minimum impedance, while in parallel circuits, it leads to maximum impedance.

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