Conductors and Insulators — Question 4

Section 21-2 · Physics pages 3398–3399

Question 4 Unequal conducting spheres need not share charge equally Two widely separated metal spheres of radii RA = 2.0 cm and RB = 6.0 cm carry total charge +16 nC. A long thin wire connects them. Neglect the charge on the wire and mutual influence on the spheres. For this exercise use the supplied equilibrium rule QA/RA = QB/RB. RA RB Schematic; labels, not drawing lengths, specify the data. (a) Find the final sphere charges and compare with equal sharing. (b) Using σ = Q/(4πR2) for each approximately uniform sphere, find the ratio of surface charge densities. Explain how the smaller sphere can carry less charge but have greater density.
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Question 4 - Solution Unequal conducting spheres need not share charge equally RA RB (a) Method and calculation QB = RB RA QA = 3QA, QA + QB = 16 nC. QA = 4.0 nC, QB = 12.0 nC. (b) Interpretation and further calculation σA σB = QA QB (RB RA )2 = 1 3(3)2 = 3. Q ∝R, σ ∝R−1 at the stated equilibrium. Area grows as R2, faster than the equilibrium charge grows with radius. Physical check The supplied ratio assumes widely separated spheres; nearby conductors alter each other charge distributions.

Question 4

Unequal conducting spheres need not share charge equally

Two widely separated metal spheres of radii RA=2.0R_A=2.0 cm and RB=6.0R_B=6.0 cm carry total charge +16+16 nC. A long thin wire connects them. Neglect the charge on the wire and mutual influence on the spheres. For this exercise use the supplied equilibrium rule QA/RA=QB/RBQ_A/R_A=Q_B/R_B.

Diagram shown in the original SVG worksheet.

  1. Find the final sphere charges and compare with equal sharing.

  2. Using σ=Q/(4πR2)\sigma=Q/(4\pi R^2) for each approximately uniform sphere, find the ratio of surface charge densities. Explain how the smaller sphere can carry less charge but have greater density.

Question 4 - Solution

Unequal conducting spheres need not share charge equally

Diagram shown in the original SVG worksheet.

(a) Method and calculation

QB=RBRAQA=3QA,QA+QB=16nC.Q_B=\frac{R_B}{R_A}Q_A=3Q_A,\quad Q_A+Q_B=16\,\mathrm{nC}.QA=4.0nC,QB=12.0nC.Q_A=4.0\,\mathrm{nC},\quad Q_B=12.0\,\mathrm{nC}.

(b) Interpretation and further calculation

σAσB=QAQB(RBRA)2=13(3)2=3.\frac{\sigma_A}{\sigma_B}=\frac{Q_A}{Q_B}\left(\frac{R_B}{R_A}\right)^2=\frac13(3)^2=3.Q∝R,σ∝R−1at the stated equilibrium.Q\propto R,\qquad\sigma\propto R^{-1}\quad\text{at the stated equilibrium}.Area grows as R2R^2, faster than the equilibrium charge grows with radius.

Physical check

The supplied ratio assumes widely separated spheres; nearby conductors alter each other charge distributions.