Alternating Current — Question 8

Section 31-5 · Physics pages 5066–5067

Question 8 Different harmonics add their mean-square contributions independently A current is i(t) = 3 cos ωt + 4 sin 2ωt amperes through a 2.00-ohm resistor. Average over the fundamental period. ωt i Schematic; labels, not drawing lengths, specify the data. (a) Compute rms current using harmonic orthogonality. (b) Find mean heating and compare with a 5.00-A peak sinusoid.
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Question 8 - Solution Different harmonics add their mean-square contributions independently ωt i (a) Method and calculation ⟨i2⟩= 9⟨cos2 ωt⟩+ 16⟨sin2 2ωt⟩+ 24⟨cos ωt sin 2ωt⟩. I2 rms = (9 + 16)/2 = 12.5 A2 . (b) Interpretation and further calculation ⟨P⟩= 2(12.5) = 25.0 W . Irms,sine = 5/ √ 2 = Irms ⇒Psine = P . Physical check Equal rms heating does not mean equal waveforms or equal instantaneous peaks.

Question 8

Different harmonics add their mean-square contributions independently

A current is i(t)=3cos⁡ωt+4sin⁡2ωti(t)=3\cos\omega t+4\sin2\omega t amperes through a 2.00-ohm resistor. Average over the fundamental period.

Diagram shown in the original SVG worksheet.

  1. Compute rms current using harmonic orthogonality.

  2. Find mean heating and compare with a 5.00-A peak sinusoid.

Question 8 - Solution

Different harmonics add their mean-square contributions independently

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨i2⟩=9⟨cos⁡2ωt⟩+16⟨sin⁡22ωt⟩+24⟨cos⁡ωtsin⁡2ωt⟩.\langle i^2\rangle=9\langle\cos^2\omega t\rangle+16\langle\sin^22\omega t\rangle+24\langle\cos\omega t\sin2\omega t\rangle.Irms2=(9+16)/2=12.5A2.\boxed{I_{\mathrm{rms}}^2=(9+16)/2=12.5\,A^2}.

(b) Interpretation and further calculation

⟨P⟩=2(12.5)=25.0W.\boxed{\langle P\rangle=2(12.5)=25.0\,W}.Irms,sine=5/2=Irms⇒Psine=P.I_{\mathrm{rms,sine}}=5/\sqrt2=I_{\mathrm{rms}}\Rightarrow\boxed{P_{\mathrm{sine}}=P}.

Physical check

Equal rms heating does not mean equal waveforms or equal instantaneous peaks.