Capacitors in Parallel and in Series — Question 6

Section 25-3 · Physics pages 4062–4063

Question 6 Trapped junction charge breaks the usual equality of series charges A capacitor C joins A to M and a capacitor 2C joins M to B. Set VA=V>0 and VB=0. The isolated junction M has prescribed net charge QM = CV . A B C1 C2 M Schematic; labels, not drawing lengths, specify the data. (a) Find VM from junction charge conservation. (b) Find the signed charges on the A plate and on the M plate facing B, and explain their unequal magnitudes.
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Question 6 - Solution Trapped junction charge breaks the usual equality of series charges A B C1 C2 M (a) Method and calculation QM = C(VM −VA) + 2C(VM −VB). CV = 3CVM −CV ⇒VM = 2V/3. (b) Interpretation and further calculation qA = C(V −VM) = CV/3. qM→B = 2CVM = 4CV/3, (−CV/3) + (4CV/3) = QM. Physical check An isolated junction conserves its net charge; zero net charge is an additional assumption, not a universal rule.

Question 6

Trapped junction charge breaks the usual equality of series charges

A capacitor C joins A to M and a capacitor 2C joins M to B. Set VA=V>0 and VB=0. The isolated junction M has prescribed net charge QM=CVQ_M=CV.

Diagram shown in the original SVG worksheet.

  1. Find VM from junction charge conservation.

  2. Find the signed charges on the A plate and on the M plate facing B, and explain their unequal magnitudes.

Question 6 - Solution

Trapped junction charge breaks the usual equality of series charges

Diagram shown in the original SVG worksheet.

(a) Method and calculation

QM=C(VM−VA)+2C(VM−VB).Q_M=C(V_M-V_A)+2C(V_M-V_B).CV=3CVM−CV⇒VM=2V/3.CV=3CV_M-CV\Rightarrow V_M=2V/3.

(b) Interpretation and further calculation

qA=C(V−VM)=CV/3.q_A=C(V-V_M)=CV/3.qM→B=2CVM=4CV/3,(−CV/3)+(4CV/3)=QM.q_{M\to B}=2CV_M=4CV/3,\quad(-CV/3)+(4CV/3)=Q_M.

Physical check

An isolated junction conserves its net charge; zero net charge is an additional assumption, not a universal rule.