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5 - N u m e r i c a l   7

Problem

For a series RLC circuit with a 40.0 Ω40.0 \, \Omega resistor, a 3.00 mH3.00 \, \mathrm{mH} inductor, and a 5.00 μF5.00 \, \mu\mathrm{F} capacitor: (a) Calculate the resonant frequency.
(b) Determine the RMS current at resonance if Vrms=120 VV_{\mathrm{rms}} = 120 \, \mathrm{V}.

Data

  • Resistance: R=40.0 ΩR = 40.0 \, \Omega
  • Inductance: L=3.00 mH=3.00×10−3 HL = 3.00 \, \mathrm{mH} = 3.00 \times 10^{-3} \, \mathrm{H}
  • Capacitance: C=5.00 μF=5.00×10−6 FC = 5.00 \, \mu\mathrm{F} = 5.00 \times 10^{-6} \, \mathrm{F}
  • RMS Voltage: Vrms=120 VV_{\mathrm{rms}} = 120 \, \mathrm{V}

Prerequisite Concepts

  1. Resonant frequency for a series RLC circuit:
f0=12Ï€LC f_0 = \frac{1}{2\pi \sqrt{LC}}
  1. At resonance, the circuit behaves as purely resistive, and the impedance Z=RZ = R. The RMS current is given by:
Irms=VrmsR I_{\mathrm{rms}} = \frac{V_{\mathrm{rms}}}{R}

Solution

Part (a): Calculate the Resonant Frequency

f0=12Ï€LCf_0 = \frac{1}{2\pi \sqrt{LC}}

Substitute the given values:

f0=12×3.14×(3.00×10−3 H)×(5.00×10−6 F)f_0 = \frac{1}{2 \times 3.14 \times \sqrt{(3.00 \times 10^{-3} \, \mathrm{H}) \times (5.00 \times 10^{-6} \, \mathrm{F})}} f0=16.28×1.50×10−8f_0 = \frac{1}{6.28 \times \sqrt{1.50 \times 10^{-8}}} f0=16.28×1.225×10−4f_0 = \frac{1}{6.28 \times 1.225 \times 10^{-4}} f0=17.691×10−4f_0 = \frac{1}{7.691 \times 10^{-4}} f0=1.30×103 Hzf_0 = 1.30 \times 10^{3} \, \mathrm{Hz}

Part (b): Calculate the RMS Current at Resonance

At resonance, the circuit impedance Z=RZ = R. The RMS current is:

Irms=VrmsRI_{\mathrm{rms}} = \frac{V_{\mathrm{rms}}}{R}

Substitute the values:

Irms=120 V40.0 ΩI_{\mathrm{rms}} = \frac{120 \, \mathrm{V}}{40.0 \, \Omega} Irms=3.00 AI_{\mathrm{rms}} = 3.00 \, \mathrm{A}

Answer

  • Resonant Frequency: f0=1.30 kHzf_0 = 1.30 \, \mathrm{kHz}
  • RMS Current at Resonance: Irms=3.00 AI_{\mathrm{rms}} = 3.00 \, \mathrm{A}