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MHT CET 2026 (15 May, Shift 1) · Rotating Conductors & AC Generator

Rotating Conductors & AC Generator question from MHT CET 2026 (15 May, Shift 1)

Q2MHT CET 2026 · 15 MAY · SHIFT 1Medium

Rotating Conductors & AC Generator

A conducting rod AC of length 4L4L is rotated counter-clockwise about a point O in a uniform magnetic field BB directed into the paper. If AO=LAO = L and OC=3LOC = 3L then (ω\omega = angular speed)

Figure

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Answer: (c)

ACOL3LV_O − V_A = BωL²/2V_O − V_C = 9BωL²/2
  1. For a rod rotating about a pivot, the emf between the pivot and a point at distance rr is 12Bωr2\frac{1}{2}B\omega r^2.
  2. With B⃗\vec B into the page and counter-clockwise rotation, qv⃗×B⃗q\vec v \times \vec B pushes positive charge towards O, so O is at the higher potential.
  3. VO−VA=12BωL2V_O - V_A = \frac{1}{2}B\omega L^2, VO−VC=12Bω(3L)2=92BωL2V_O - V_C = \frac{1}{2}B\omega(3L)^2 = \frac{9}{2}B\omega L^2
  4. VA−VC=(VO−VC)−(VO−VA)=92BωL2−12BωL2=4BωL2V_A - V_C = (V_O - V_C) - (V_O - V_A) = \frac{9}{2}B\omega L^2 - \frac{1}{2}B\omega L^2 = 4B\omega L^2
  5. So the answer is (c) VA−VC=4BωL2V_A - V_C = 4B\omega L^2.
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