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Question #43358

Difficulty: 8/10 | 🟢 Free

The Question

An electrostatic potentiometer is constructed using a long cylindrical capacitor of inner radius aa and outer radius bb. The region between the cylinders (a≤r≤ba \le r \le b) is filled with a non-uniform dielectric medium whose relative permittivity varies with radial distance rr as κ(r)=κ0ra\kappa(r) = \kappa_0 \frac{r}{a}, where κ0\kappa_0 is a positive constant. A constant DC voltage source maintains the inner cylinder at a potential V0V_0 and the outer cylinder at ground (0 V0\text{ V}). A radial probe is used to find a null point where the local potential balances an ideal cell of EMF E=V02\mathcal{E} = \frac{V_0}{2} connected between the probe and the grounded outer cylinder. At what radial distance r0r_0 from the central axis will the null point be obtained?

Options

  • A.

    a+b2\frac{a+b}{2}

  • B.

    ab\sqrt{ab}

  • C.

    2aba+b\frac{2ab}{a+b}

  • D.

    a2+b2a+b\frac{a^2+b^2}{a+b}

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Correct Answer

Step-by-Step Solution

Explanation

How the Examiner Thinks

Intuition_Breaker

Train your brain to resist "obvious" answers that are designed to deceive your intuition.

Concepts Behind This Question

Potentiometer Sensitivity|Gauss Law Applicability|Dielectric Polarization Logic

Why This Question Is Tricky

Common Mistakes

This question tests the misapplication of potential gradient linearity in non-uniform media and geometries.

Students often assume a linear potential drop V(r)∝rV(r) \propto r (yielding the arithmetic mean a+b2\frac{a+b}{2}) as in a standard wire potentiometer, completely ignoring the cylindrical geometry.

A secondary trap is assuming a standard logarithmic potential drop V(r)∝ln⁡(r)V(r) \propto \ln(r) (yielding the geometric mean ab\sqrt{ab}), which accounts for the geometry but ignores the spatially varying dielectric constant.

The correct approach requires deriving the local electric field from Gauss's Law for the displacement field (∇⋅D⃗=ρfree\nabla \cdot \vec{D} = \rho_{\text{free}}) and integrating E(r)=D(r)/ϵ(r)E(r) = D(r)/\epsilon(r) to find the true non-linear potential distribution, which in this specific case yields the harmonic mean.

Quick Facts About This Question

Question Information

SubjectPhysics
ChapterCurrent Electricity - Class 12
ConceptPotentiometer Sensitivity
Difficulty8
Cognitive Load7
Target Solve Time160 sec
AccessFree