A Charged Isolated Conductor — Question 2

Section 23-5 · Physics pages 3714–3715

Question 2 An off-center cavity charge fixes induced totals without fixing their density An isolated conductor has one closed cavity containing a fixed charge q = +3.00 nC, displaced from the cavity center and not touching the wall. The metal itself has net charge Qc = −1.00 nC. q Cross-section of a conducting shell in electrostatic equilibrium; shaded material is metal. (a) Use a Gaussian surface entirely within the metal and surrounding the cavity to find the total inner-wall charge. Then find the outer-surface charge. (b) The charge moves within the cavity without contact. Determine which induced totals stay fixed, and explain whether the inner surface density must remain unchanged.
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Question 2 - Solution An off-center cavity charge fixes induced totals without fixing their density q (a) Method and calculation Emetal = 0 ⇒Φmetal = 0 ⇒q + Qinner = 0. Qinner = −3.00 nC, Qouter = Qc −Qinner = +2.00 nC. (b) Interpretation and further calculation Qinner′ = −q = Qinner, Qouter′ = Qc + q = Qouter. ∫ inner σ dA = −q. The integral is fixed, but local surface density generally redistributes as the cavity charge moves. Physical check Charge inside the cavity belongs to the enclosed system but is not part of the specified net charge on the isolated metal.

Question 2

An off-center cavity charge fixes induced totals without fixing their density

An isolated conductor has one closed cavity containing a fixed charge q=+3.00q=+3.00 nC, displaced from the cavity center and not touching the wall. The metal itself has net charge Qc=−1.00Q_c=-1.00 nC.

Diagram shown in the original SVG worksheet.

  1. Use a Gaussian surface entirely within the metal and surrounding the cavity to find the total inner-wall charge. Then find the outer-surface charge.

  2. The charge moves within the cavity without contact. Determine which induced totals stay fixed, and explain whether the inner surface density must remain unchanged.

Question 2 - Solution

An off-center cavity charge fixes induced totals without fixing their density

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑬metal=0⇒Φmetal=0⇒q+Qinner=0.\mathbf E_{\mathrm{metal}}=0\Rightarrow\Phi_{\mathrm{metal}}=0\Rightarrow q+Q_{\mathrm{inner}}=0.Qinner=−3.00nC,Qouter=Qc−Qinner=+2.00nC.Q_{\mathrm{inner}}=-3.00\,\mathrm{nC},\quad Q_{\mathrm{outer}}=Q_c-Q_{\mathrm{inner}}=+2.00\,\mathrm{nC}.

(b) Interpretation and further calculation

Qinner′=−q=Qinner,Qouter′=Qc+q=Qouter.Q_{\mathrm{inner}}\prime=-q=Q_{\mathrm{inner}},\quad Q_{\mathrm{outer}}\prime=Q_c+q=Q_{\mathrm{outer}}.∫innerσdA=−q.\int_{\mathrm{inner}}\sigma\,dA=-q.The integral is fixed, but local surface density generally redistributes as the cavity charge moves.

Physical check

Charge inside the cavity belongs to the enclosed system but is not part of the specified net charge on the isolated metal.