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Syllabus
🩺 NEET UG
Subject:Physics Syllabus

Electromagnetic Induction & Alternating Current

Syllabus Unit: Electrodynamics

Why it matters

Chapter overview

Electromagnetic induction shows that a changing magnetic flux creates an EMF (Faraday's law) in a direction that always opposes the change producing it (Lenz's law) — the working principle behind generators, transformers, and self and mutual inductance. When the induced or applied EMF alternates, AC circuit theory — impedance, phasors, resonance and power factor — determines how current, voltage and power behave in circuits containing resistors, inductors and capacitors together.

Physics Syllabus Electrodynamics 25%–30% weightage
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N SMoving magnet → induced EMFFaraday's & Lenz's Law Lab

1Faraday's & Lenz's Laws

Faraday's law quantifies the EMF induced by a changing magnetic flux; Lenz's law fixes its direction by demanding that induced effects always oppose the very change producing them.

Learning Objectives

  • State Faraday's law of EM induction, EMF = −N dΦ/dt.
  • State Lenz's law and explain it as a consequence of the conservation of energy.
  • Identify the three ways magnetic flux can change: changing B, changing A, or changing the angle θ.
  • Calculate the motional EMF induced in a rod moving through a magnetic field, EMF = Bvl.

Key Terms

Magnetic Flux (Φ)Φ = B·A = BAcosθ, the 'amount' of magnetic field passing through a surface, measured in weber (Wb).
Faraday's LawInduced EMF = −N dΦ/dt; the induced EMF is proportional to the rate of change of flux linkage across N turns.
Lenz's LawThe induced current flows in a direction that opposes the change in flux that produced it — the source of the minus sign in Faraday's law.
Motional EMFEMF induced in a conductor moving through a magnetic field, EMF = Bvl sinθ, derivable from the magnetic force on the rod's free charges.

Electromagnetic induction was discovered through a subtle but crucial fact: only a **changing** magnetic flux induces an EMF — a steady, unchanging flux, however large, induces nothing at all.

Φ = B A cosθ EMF = −N dΦ/dt

Three ways to change flux

  • Change B — moving a magnet toward or away from a coil.
  • Change A — a loop's area expanding or shrinking, or a rod sliding on rails.
  • Change θ — rotating a coil within a fixed field, the basis of the AC generator.

Lenz's law — the direction

The induced current always opposes the change in flux that caused it: if flux is increasing, the induced current creates a field opposing the increase; if flux is decreasing, it creates a field reinforcing it. This is why work must be done to push a magnet toward a coil — the induced current's own field pushes back. Lenz's law is simply energy conservation in disguise.

Common MistakeTrap: Lenz's law opposes the CHANGE in flux, not the flux itself — a large but steady, unchanging flux induces zero EMF.

Motional EMF

EMF = B v l sinθ
Key PointMotional EMF can be derived directly from the magnetic force qv×B pushing free electrons in the moving rod to one end, building a charge separation until the electric force balances the magnetic one — the same physics as Faraday's law applied to a changing area.