Power in Electric Circuits — Question 2

Section 26-6 · Physics pages 4254–4255

Question 2 A zero-mean current still heats a resistor A constant resistor R carries I(t) = Id + Ia cos ωt. Average over a whole number of periods. t Schematic; labels, not drawing lengths, specify the data. (a) Derive average power and root-mean-square current. (b) Compare equal-peak sinusoidal and symmetric square-wave currents of peak magnitude Ia and zero mean.
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Question 2 - Solution A zero-mean current still heats a resistor t (a) Method and calculation ⟨I2⟩= I2 d + 2IdIa⟨cos ωt⟩+ I2 a⟨cos2 ωt⟩= I2 d + I2 a/2. P = R(I2 d + I2 a/2), Irms = √ I2 d + I2a/2. (b) Interpretation and further calculation Psin = RI2 a/2, P□= RI2 a. P□/Psin = 2, ⟨I⟩= 0 for both. Physical check Resistive heating depends on the mean square, not the signed mean current.

Question 2

A zero-mean current still heats a resistor

A constant resistor R carries I(t)=Id+Iacos⁡ωtI(t)=I_d+I_a\cos\omega t. Average over a whole number of periods.

Diagram shown in the original SVG worksheet.

  1. Derive average power and root-mean-square current.

  2. Compare equal-peak sinusoidal and symmetric square-wave currents of peak magnitude IaI_a and zero mean.

Question 2 - Solution

A zero-mean current still heats a resistor

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨I2⟩=Id2+2IdIa⟨cos⁡ωt⟩+Ia2⟨cos⁡2ωt⟩=Id2+Ia2/2.\langle I^2\rangle=I_d^2+2I_dI_a\langle\cos\omega t\rangle+I_a^2\langle\cos^2\omega t\rangle=I_d^2+I_a^2/2.P¯=R(Id2+Ia2/2),Irms=Id2+Ia2/2.\overline P=R(I_d^2+I_a^2/2),\quad I_{\mathrm{rms}}=\sqrt{I_d^2+I_a^2/2}.

(b) Interpretation and further calculation

Psin=RIa2/2,P▫=RIa2.P_{\sin}=RI_a^2/2,\quad P_{\square}=RI_a^2.P▫/Psin=2,⟨I⟩=0for both.P_{\square}/P_{\sin}=2,\quad\langle I\rangle=0\ \text{for both}.

Physical check

Resistive heating depends on the mean square, not the signed mean current.