Three Simple Circuits — Question 2

Section 31-7 · Physics pages 5094–5095

Question 2 A capacitor current leads because it tracks the voltage slope An ideal capacitor of C = 4.00 µF has v = 20.0 cos(500t) volts, using passive current direction. ∼ v i C Schematic; labels, not drawing lengths, specify the data. (a) Find i(t), rms current, and capacitive reactance. (b) Find capacitor energy when voltage is zero and when current is zero.
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Question 2 - Solution A capacitor current leads because it tracks the voltage slope ∼ v i C (a) Method and calculation i = C ˙v = −ωCVp sin ωt. i = −.0400 sin(500t) A, Irms = .0282843 A, XC = 1/(ωC) = 500 Ω. (b) Interpretation and further calculation UC = 1 2Cv2, v = 0 ⇒UC = 0. i = 0 : UC = 1 2CV 2 p = .800 mJ . Physical check The current reaches its extrema at voltage zeros; a large current need not mean large stored electric energy.

Question 2

A capacitor current leads because it tracks the voltage slope

An ideal capacitor of C=4.00μFC=4.00\,\mu F has v=20.0cos⁡(500t)v=20.0\cos(500t) volts, using passive current direction.

Diagram shown in the original SVG worksheet.

  1. Find i(t), rms current, and capacitive reactance.

  2. Find capacitor energy when voltage is zero and when current is zero.

Question 2 - Solution

A capacitor current leads because it tracks the voltage slope

Diagram shown in the original SVG worksheet.

(a) Method and calculation

i=Cv̇=−ωCVpsin⁡ωt.i=C\dot v=-\omega CV_p\sin\omega t.i=−.0400sin⁡(500t)A,Irms=.0282843A,XC=1/(ωC)=500Ω.\boxed{i=-.0400\sin(500t)\,A,\quad I_{\mathrm{rms}}=.0282843\,A,\quad X_C=1/(\omega C)=500\,\Omega}.

(b) Interpretation and further calculation

UC=12Cv2,v=0⇒UC=0.U_C=\tfrac12Cv^2,\quad v=0\Rightarrow U_C=0.i=0:UC=12CVp2=.800mJ.\boxed{i=0:\quad U_C=\tfrac12CV_p^2=.800\,mJ}.

Physical check

The current reaches its extrema at voltage zeros; a large current need not mean large stored electric energy.