(1) Three concentric spherical shells have radii a, b and c (a < b < c) and have surface charge densities σ, − σ and σ respectively. If VA, VB and VC denote the potentials of the three shells, then for c = a + b, we have
(1) VC = VB ≠ VA
(2) VC ≠ VB ≠ VA
(3) VC = VB = VA
(4) VC = VA ≠ VB
The potential V of a spherical shell of radius r having surface charge density σ is given by
V = (1/4πε0)(4πr2σ/r) = σr/ε0 where ε0 is the permittivity of free space.
Potential VA of the shell A is given by
VA = σa/ε0 – σb/ε0 + σc/ε0 = (σ/ε0)[c – (b – a)]
Potential VB of the shell B is given by
VB = – σb/ε0 + (1/4πε0)(4πa2σ/b) + σc/ε0
Or, VB = σ/ε0 [c – (b2 – a2)/b]
Potential VC of the shell C is given by
VC = σc/ε0 – (1/4πε0)(4πb2σ/c) + (1/4πε0)(4πa2σ/c)
Or, VC = σ/ε0 [c – (b2 – a2)/c] = σ/ε0 [c – (b + a)(b– a)/c]
Since c = a + b we obtain
VC = σ/ε0 [c – (b– a)]
The correct option therefore is VC = VA ≠ VB.
(2) Three capacitors each of capacitance C and of breakdown voltage V are joined in series. The capacitance and breakdown voltage of the combination will be
(1) 3 C, V/3
(2) C/3, 3 V
(3) 3 C, 3V
(4) C/3, V/3
This is a very simple question. The effective calacitance Ceff of the combination of three capacitors in series is given by the reciprocal relation,
1/Ceff = 1/C1 +1/C2 +1/C3
Here C1 = C2 = C3 = C so that Ceff = C/3
The breakdown voltage Veff for the series combination is the sum of the individual breakdown voltages:
Veff = 3V
(3) The electric potential at a point (x, y, z) is given by V = − x2y − xz3 + 4. The electric field E at that point is:
(1) E = i 2xy + j (x2 + y2) + k (3xz − y2)
(2) E = i z 3 + j xyz + k z2
(3) E = i (2xy − z3) + j xy2 + k 3z2x
(4) E = i (2xy + z3) + j x2 + k 3xz2
The electric field E is the negative gradient of potential:
E = − ∂V/∂r = − (i ∂V/∂x + j ∂V/∂y + k ∂V/∂z)
This gives E = i (2xy + z3) + j x2 + k 3xz2 as given in option (4).
You will find similar useful multiple choice questions (with solution) in electrostatics at aphysicsresources and at physicsplus
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