LC Oscillations, Quantitatively — Question 9

Section 31-3 · Physics pages 5028–5029

Question 9 Signed transported charge vanishes over a cycle while total passage does not An ideal LC loop has q = Q cos ωt and i = ˙q. Define signed transported charge as ∫i dt and total passage as ∫|i|dt. ωt i/Imax Schematic; labels, not drawing lengths, specify the data. (a) Find both quantities over one full cycle. (b) Find the cycle-average current magnitude and compare it with rms current.
Show solutionHide solution
Question 9 - Solution Signed transported charge vanishes over a cycle while total passage does not ωt i/Imax (a) Method and calculation ∫T 0 i dt = q(T) −q(0) = 0 . ∫T 0 |i|dt = Q ∫2π 0 | sin θ|dθ = 4Q . (b) Interpretation and further calculation ⟨|i|⟩= 4Q/T = 2Imax/π, Irms = Imax/ √ 2. ⟨|i|⟩/Irms = 2 √ 2/π = .900316 . Physical check Zero signed transfer does not imply that no charge moved through the wire.

Question 9

Signed transported charge vanishes over a cycle while total passage does not

An ideal LC loop has q=Qcos⁡ωtq=Q\cos\omega t and i=q̇i=\dot q. Define signed transported charge as ∫idt\int i\,dt and total passage as ∫|i|dt\int|i|dt.

Diagram shown in the original SVG worksheet.

  1. Find both quantities over one full cycle.

  2. Find the cycle-average current magnitude and compare it with rms current.

Question 9 - Solution

Signed transported charge vanishes over a cycle while total passage does not

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∫0Tidt=q(T)−q(0)=0.\int_0^Ti\,dt=q(T)-q(0)=\boxed{0}.∫0T|i|dt=Q∫02π|sin⁡θ|dθ=4Q.\int_0^T|i|dt=Q\int_0^{2\pi}|\sin\theta|d\theta=\boxed{4Q}.

(b) Interpretation and further calculation

⟨|i|⟩=4Q/T=2Imax/π,Irms=Imax/2.\langle|i|\rangle=4Q/T=2I_{\max}/\pi,\quad I_{\mathrm{rms}}=I_{\max}/\sqrt2.⟨|i|⟩/Irms=22/π=.900316.\boxed{\langle|i|\rangle/I_{\mathrm{rms}}=2\sqrt2/\pi=.900316}.

Physical check

Zero signed transfer does not imply that no charge moved through the wire.