Three Simple Circuits — Question 3

Section 31-7 · Physics pages 5096–5097

Question 3 An ideal inductor retains a DC current set by its initial condition An ideal inductor L has applied voltage v = Vp cos ωt and initial current Idc at t=0. No resistance is present. ∼ v i L Schematic; labels, not drawing lengths, specify the data. (a) Integrate the voltage law and identify the sinusoidal current component. (b) Find total rms current and mean magnetic energy.
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Question 3 - Solution An ideal inductor retains a DC current set by its initial condition ∼ v i L (a) Method and calculation L˙i = Vp cos ωt ⇒i = Idc + Vp ωL sin ωt . Iac,p = Vp/(ωL), XL = ωL. (b) Interpretation and further calculation I2 rms = I2 dc + 1 2 ( Vp ωL )2 . ⟨UL⟩= 1 2LI2 dc + V 2 p 4ω2L . Physical check The ideal inductor has no mechanism to remove its integration constant; a sinusoidal-only assumption must be stated.

Question 3

An ideal inductor retains a DC current set by its initial condition

An ideal inductor L has applied voltage v=Vpcos⁡ωtv=V_p\cos\omega t and initial current Idc at t=0. No resistance is present.

Diagram shown in the original SVG worksheet.

  1. Integrate the voltage law and identify the sinusoidal current component.

  2. Find total rms current and mean magnetic energy.

Question 3 - Solution

An ideal inductor retains a DC current set by its initial condition

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Li̇=Vpcos⁡ωt⇒i=Idc+VpωLsin⁡ωt.L\dot i=V_p\cos\omega t\Rightarrow\boxed{i=I_{\mathrm{dc}}+\frac{V_p}{\omega L}\sin\omega t}.Iac,p=Vp/(ωL),XL=ωL.I_{{\mathrm{ac}},p}=V_p/(\omega L),\quad X_L=\omega L.

(b) Interpretation and further calculation

Irms2=Idc2+12(VpωL)2.\boxed{I_{\mathrm{rms}}^2=I_{\mathrm{dc}}^2+\frac12\left(\frac{V_p}{\omega L}\right)^2}.⟨UL⟩=12LIdc2+Vp24ω2L.\boxed{\langle U_L\rangle=\tfrac12LI_{\mathrm{dc}}^2+\frac{V_p^2}{4\omega^2L}}.

Physical check

The ideal inductor has no mechanism to remove its integration constant; a sinusoidal-only assumption must be stated.