Electromagnetic Induction: Tricky Questions Solved (1)

easy 2 min read

Question

A rod of length L=0.5L = 0.5 m moves with constant velocity v=4v = 4 m/s perpendicular to a uniform magnetic field B=0.5B = 0.5 T. The rod slides on two parallel frictionless rails connected through a resistance R=2ΩR = 2\,\Omega. Find the induced emf, the current, the force needed to keep the rod moving at constant velocity, and the power dissipated. Also verify energy balance.

Solution — Step by Step

ε=BLv=0.5×0.5×4=1V\varepsilon = BLv = 0.5 \times 0.5 \times 4 = 1 \, \text{V} I=ε/R=1/2=0.5AI = \varepsilon / R = 1/2 = 0.5 \, \text{A}

The current-carrying rod in the field experiences:

Fmag=BIL=0.5×0.5×0.5=0.125NF_{mag} = BIL = 0.5 \times 0.5 \times 0.5 = 0.125 \, \text{N}

This opposes motion (Lenz’s law), so the external force needed is Fext=0.125F_{ext} = 0.125 N in the direction of motion.

Pext=Fext×v=0.125×4=0.5WP_{ext} = F_{ext} \times v = 0.125 \times 4 = 0.5 \, \text{W} PR=I2R=(0.5)2×2=0.5WP_{R} = I^2 R = (0.5)^2 \times 2 = 0.5 \, \text{W}

Energy in = energy out. Balance verified.

Final answer: ε=1\varepsilon = 1 V, I=0.5I = 0.5 A, F=0.125F = 0.125 N, P=0.5P = 0.5 W.

Why This Works

The motional emf BLvBLv comes from the magnetic force on free electrons inside the moving rod. Once current flows, the same field exerts a retarding force on the rod, perfectly converting mechanical work into electrical heat.

This is energy conservation in action — Lenz’s law is just a way to state that you cannot get electrical energy for free.

Alternative Method

Use ε=dΦ/dt\varepsilon = -d\Phi/dt. Flux through the loop =B×(area)=B×Lx= B \times (\text{area}) = B \times Lx where xx is the rod’s position. Then dΦ/dt=BLdx/dt=BLvd\Phi/dt = BL\, dx/dt = BLv. Same emf.

Students often forget the sign of FmagF_{mag} — it must oppose vv (Lenz’s law). If you draw the force in the direction of motion, you would conclude the rod accelerates by itself, which violates energy conservation.

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