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5 - N u m e r i c a l   8

Problem

A coil of pure inductance 318mH318 \, \mathrm{mH} is connected in series with a pure resistance of 75Ω75 \, \Omega. The voltage across the resistor is 150V150 \, \mathrm{V}, and the frequency of the power supply is 50Hz50 \, \mathrm{Hz}. Calculate the voltage of the power supply and the phase angle.

Data

  • Inductance: L=318mH=318×103HL = 318 \, \mathrm{mH} = 318 \times 10^{-3} \, \mathrm{H}
  • Resistance: R=75ΩR = 75 \, \Omega
  • AC frequency: f=50Hzf = 50 \, \mathrm{Hz}
  • Voltage across the resistor: VR=150VV_R = 150 \, \mathrm{V}

Prerequisite Concepts

  1. Inductive Reactance:
XL=2πfL X_L = 2 \pi f L
  1. Impedance in an R-L Series Circuit:
Z=R2+XL2 Z = \sqrt{R^2 + X_L^2}
  1. Current through the Resistor:
I=VRR I = \frac{V_R}{R}
  1. Supply Voltage:
V=IZ V = I Z
  1. Phase Angle:
θ=tan1(XLR) \theta = \tan^{-1} \left(\frac{X_L}{R}\right)

Solution

Step 1: Calculate the Inductive Reactance

XL=2πfLX_L = 2 \pi f L XL=2×3.14×50Hz×318×103HX_L = 2 \times 3.14 \times 50 \, \mathrm{Hz} \times 318 \times 10^{-3} \, \mathrm{H} XL=99.852ΩX_L = 99.852 \, \Omega

Step 2: Calculate the Current through the Resistor

I=VRRI = \frac{V_R}{R} I=150V75ΩI = \frac{150 \, \mathrm{V}}{75 \, \Omega} I=2.00AI = 2.00 \, \mathrm{A}

Step 3: Calculate the Total Impedance

Z=R2+XL2Z = \sqrt{R^2 + X_L^2} Z=(75Ω)2+(99.852Ω)2Z = \sqrt{(75 \, \Omega)^2 + (99.852 \, \Omega)^2} Z=5625+9970.63Z = \sqrt{5625 + 9970.63} Z=15595.63=124.88ΩZ = \sqrt{15595.63} = 124.88 \, \Omega

Step 4: Calculate the Supply Voltage

V=IZV = I Z V=2.00A×124.88ΩV = 2.00 \, \mathrm{A} \times 124.88 \, \Omega V=249.76V250VV = 249.76 \, \mathrm{V} \approx 250 \, \mathrm{V}

Step 5: Calculate the Phase Angle

θ=tan1(XLR)\theta = \tan^{-1} \left(\frac{X_L}{R}\right) θ=tan1(99.852Ω75Ω)\theta = \tan^{-1} \left(\frac{99.852 \, \Omega}{75 \, \Omega}\right) θ=53.06\theta = 53.06^\circ

Answer

  • Supply Voltage: V=250VV = 250 \, \mathrm{V}
  • Phase Angle: θ=53.06\theta = 53.06^\circ