Complete NEET prep for Electromagnetic Induction: magnetic flux, Faraday's law, Lenz's law, motional EMF, eddy currents, self and mutual induction, energy stored in an inductor. NCERT-aligned notes, 30+ PYQs and live interactive widgets. Built for NEET 2027.
Chapter Notes
Complete NCERT-aligned notes with KaTeX equations, worked NEET problems and inline interactive widgets.
NEET Questions
30+ NEET previous year questions with full step-by-step solutions, grouped by topic.
Interactive Learning
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Magnetic flux Phi equals B dot A; unit weber
Faraday's law: induced EMF equals minus d Phi over dt
Lenz's law: induced current opposes the change
Motional EMF in a rod sliding on rails: epsilon equals B L v
Eddy currents and how they cause electromagnetic damping
Self-inductance L; EMF equals minus L di over dt
Mutual inductance M between two coils
Energy stored in an inductor: half L I squared
Five worked NEET problems on every type of question
20 questions from Electromagnetic Induction across the last 5 NEET papers.
NEET 2024
4
questions
NEET 2023
4
questions
NEET 2022
4
questions
NEET 2021
4
questions
NEET 2020
4
questions
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You can expect 1 to 2 questions in NEET 2027. The chapter has high PYQ frequency. Faraday's law applications, motional EMF, Lenz's law direction, self-inductance and energy stored in an inductor are favourites.
Whenever the magnetic flux through a closed loop changes, an EMF is induced in the loop equal to minus the rate of change of flux. epsilon equals minus d Phi over dt. For N turns, multiply by N. The induced EMF drives a current if the loop is closed.
The direction of the induced current is such that it OPPOSES the change in flux that produced it. This is the meaning of the negative sign in Faraday's law. Lenz's law follows from energy conservation: if the induced current aided the change, you could create energy out of nothing.
A conducting rod of length L moving with velocity v perpendicular to a magnetic field B (with v perpendicular to L) develops EMF epsilon equals B L v across its ends. This is induced EMF without any time-varying field; the change of flux comes from the rod sweeping out new area.
Currents induced in bulk pieces of conductor by a changing flux. They form swirling loops, hence the name. Eddy currents heat up the conductor, dissipating energy. They are useful in induction stoves and magnetic braking, and undesirable in transformer cores (laminations reduce them).
When the current through a coil changes, the changing flux through itself induces a back EMF. epsilon equals minus L di over dt. L is the self-inductance, in henries (H). For a long solenoid, L equals mu_0 N squared A over length.
Building up current I from zero in an inductor requires work, which is stored in the magnetic field. U equals half L I squared. Energy density (in vacuum) is u equals B squared over (2 mu_0).
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