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AP Physics C: E&M
10.1 Electrostatics with Conductors
AdvancedMCQMathematicalConceptual18.8k
Cross section of a conducting shell with an off-center line charge.
Cross section of a conducting shell with an off-center line charge.
An uncharged, infinitely long hollow conducting cylindrical shell has inner radius \(a\) and outer radius \(b\). A thin line with uniform linear charge density \(+\lambda\) is placed inside the cavity, parallel to the central cylinder axis but displaced off-center by a distance \(d\), where \(0 < d < a\). The system is allowed to reach electrostatic equilibrium.

ChoicePotential difference \(\Delta V = V_{\text{outer}} - V_{\text{inner}}\)Total induced charge per unit length \(\int_0^{2\pi} \sigma(\theta) a \, d\theta\)
A\(0\)\(-\lambda\)
B\(0\)\(-\lambda\left(1 - \dfrac{d}{a}\right)\)
C\(\dfrac{\lambda}{2\pi\varepsilon_0}\ln\left(\dfrac{b}{a}\right)\)\(-\lambda\)
D\(\dfrac{\lambda}{2\pi\varepsilon_0}\ln\left(\dfrac{b}{a}\right)\)\(-\lambda\left(1 - \dfrac{d}{a}\right)\)

Which of the following correctly pairs the electric potential difference \(\Delta V\) between the outer and inner surfaces of the shell with the total induced surface charge per unit length on the inner cavity wall?

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