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4 - N u m e r i c a l   8

Problem

A rectangular wire loop with sides 8 cm8 \, \mathrm{cm} and 2 cm2 \, \mathrm{cm} and a small cut moves through a uniform magnetic field of magnitude 0.3 T0.3 \, \mathrm{T} directed normal to the plane of the loop. Determine:
(a) The e.m.f. induced when the velocity of the loop (v=1 cm/sv = 1 \, \mathrm{cm/s}) is normal to the longer side.
(b) The e.m.f. induced when the velocity of the loop is normal to the shorter side.
(c) The time taken in both cases.

Data

  • Length of the loop: L=8 cm=0.08 mL = 8 \, \mathrm{cm} = 0.08 \, \mathrm{m}
  • Width of the loop: W=2 cm=0.02 mW = 2 \, \mathrm{cm} = 0.02 \, \mathrm{m}
  • Magnetic field: B=0.3 TB = 0.3 \, \mathrm{T}
  • Velocity of the loop: v=1 cm/s=0.01 m/sv = 1 \, \mathrm{cm/s} = 0.01 \, \mathrm{m/s}

To find:

  1. E.m.f. induced when moving normal to the longer side (εL\varepsilon_L).
  2. E.m.f. induced when moving normal to the shorter side (εS\varepsilon_S).
  3. Time taken in both cases (Δt\Delta t).

Prerequisite Concepts

  1. Motional e.m.f. formula:
ε=BLv \varepsilon = B L v

where LL is the length of the side of the loop moving through the field.

  1. Time taken to move across the field:
t=Sv, t = \frac{S}{v},

where SS is the distance moved.

Solution

Part (a): E.m.f. Induced in the Longer Side

  1. Use the formula for motional e.m.f.:
εL=BLv. \varepsilon_L = B L v.
  1. Substituting values:
εL=0.3⋅0.08⋅0.01. \varepsilon_L = 0.3 \cdot 0.08 \cdot 0.01.
  1. Simplify:
εL=2.4×10−4 V. \varepsilon_L = 2.4 \times 10^{-4} \, \mathrm{V}.

Part (b): E.m.f. Induced in the Shorter Side

  1. Use the formula for motional e.m.f.:
εS=BWv. \varepsilon_S = B W v.
  1. Substituting values:
εS=0.3⋅0.02⋅0.01. \varepsilon_S = 0.3 \cdot 0.02 \cdot 0.01.
  1. Simplify:
εS=0.6×10−4 V. \varepsilon_S = 0.6 \times 10^{-4} \, \mathrm{V}.

Part (c): Time Taken

  1. For the longer side:
tL=Wv. t_L = \frac{W}{v}.
  1. Substituting values:
tL=0.020.01. t_L = \frac{0.02}{0.01}.
  1. Simplify:
tL=2 s. t_L = 2 \, \mathrm{s}.

Answer

  1. Induced e.m.f. when moving normal to the longer side:
εL=2.4×10−4 V. \varepsilon_L = 2.4 \times 10^{-4} \, \mathrm{V}.
  1. Induced e.m.f. when moving normal to the shorter side:
εS=0.6×10−4 V. \varepsilon_S = 0.6 \times 10^{-4} \, \mathrm{V}.
  1. Time taken in both cases:
tL=2 s. t_L = 2 \, \mathrm{s}.