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Lenz Law

Induced current opposes change in flux, conservation of energy.

Darshan N
Updated: 19 March 2026
8 min read

Lenz's law provides the physical direction rule that completes Faraday's law. While Faraday's law gives the magnitude of the induced emf, Lenz's law specifies its polarity. More deeply, Lenz's law is a direct statement of the conservation of energy in electromagnetic systems. Violating Lenz's law would mean getting electrical energy from nothing, which is impossible.

Lenz Law: Induced Current Opposes Flux ChangeCase 1: Magnet Approachingconducting loopNSmoving downB increasing downward into loopInduced I creates upward BLoop repels approaching magnetRequires force to move magnetEnergy input = electrical outputCase 2: Magnet Recedingconducting loop(arrows reversed, weaker)NSmoving upB decreasing downwardInduced I tries to maintain B downwardLoop attracts receding magnet
Figure 1: Lenz's law in action. Approaching magnet: induced current opposes approach (repulsion). Receding magnet: induced current opposes departure (attraction). Both require external work.

Core Concept Explanation

Lenz's law states that the direction of the induced emf (and hence the induced current in a closed loop) is always such that it opposes the change in magnetic flux that caused it. If the flux through a loop is increasing, the induced current flows in a direction that creates a magnetic field opposing that increase. If the flux is decreasing, the induced current flows to create a field that tries to maintain the flux.

This law is not independent of Faraday's law. It is contained within the negative sign in emf = -dΦ/dt. The negative sign is the mathematical encoding of the opposition principle. Lenz's law simply makes this physically concrete and gives a direct method to determine current direction without working through the full vector calculus.

The physical basis of Lenz's law is the conservation of energy. If the induced current aided the change instead of opposing it, the magnetic flux would increase further, inducing more current, which would increase flux more, creating a runaway loop that generates unlimited energy from nothing. This is thermodynamically impossible. Lenz's law enforces energy conservation by requiring external work to maintain any flux change against the opposing induced effects.

Mathematical Expression

Faraday's law in its signed form is emf = -dΦ/dt. The negative sign here is Lenz's law in mathematical form. To apply it correctly, one defines a positive normal direction for the loop surface using the right-hand rule. If the right-hand fingers curl in the direction of the chosen positive current direction, the thumb points in the positive normal direction. The flux Φ = ∫∫ B · n dS is then positive when B is in the positive normal direction.

When dΦ/dt > 0 (flux increasing in the positive normal direction), emf = -dΦ/dt < 0. A negative emf drives current in the negative direction (opposite to the right-hand convention), which creates a magnetic field opposing the positive normal direction (opposing the flux increase). This is exactly Lenz's law. For a coil of N turns: emf = -N·dΦ/dt and the same sign convention applies.

Practical Understanding

In eddy current braking used in trains and roller coasters, a conducting disc moves through a magnetic field. Lenz's law predicts that induced currents in the disc oppose its motion, creating a braking force. No mechanical friction is involved. The kinetic energy of the disc converts to heat in the conductor's resistance.

In metal detectors, a transmitter coil produces a changing magnetic field. When a metal object enters the field, eddy currents are induced in it by Lenz's law. These eddy currents create their own secondary field that alters the total field detected by a receiver coil. The device detects the change in mutual coupling caused by the eddy currents.

In transformer design, Lenz's law explains why the secondary voltage opposes the primary. The secondary current creates a flux that opposes the primary flux, which is why the load on a transformer is felt as increased current demand on the primary supply. Without this coupling, the primary would not know the secondary was loaded.

Example
Given:
Circular loop: radius r = 10 cm = 0.1 m, resistance R = 2 Ω
Magnetic field: B(t) = 0.5·t  T (linearly increasing, perpendicular to loop)

Why this formula applies:
dΦ/dt = A·dB/dt (area constant, B changing)
Induced emf = -N·dΦ/dt, then current I_ind = emf / R.

Formula:
Φ = B·A = B·π·r²
emf = -dΦ/dt = -πr²·(dB/dt)
I = emf / R

Substitution:
A = π × (0.1)² = π×0.01 = 3.14×10⁻² m²
dB/dt = 0.5 T/s

Calculation:
emf = -3.14×10⁻² × 0.5 = -1.57×10⁻² V = -15.7 mV
I_ind = 15.7×10⁻³ / 2 = 7.85×10⁻³ A = 7.85 mA

Direction (Lenz law):
B is increasing upward → induced I creates B downward inside loop
Using right-hand rule: induced I flows clockwise when viewed from above.

Final Answer: |emf| = 15.7 mV, I = 7.85 mA, clockwise (opposing increasing upward flux).
Exam Tip: In GATE, when asked for the direction of induced current, always use a two-step method: (1) determine if flux is increasing or decreasing, (2) apply Lenz's law to decide whether the induced B inside the loop should oppose or supplement the existing B, and then use the right-hand rule to find the current direction. Never skip either step.

Mechanism and Applications of Lenz Law

Lenz Law Applications and Energy ConservationEddy Current Brakingconducting plateeddy Imotion of plateeddy currents opposemotion: braking forceBack-emf in Motorrotor+VrefV_applied - back-emf = I·RBack-emf = k·ω (Lenz)Limits current at speedPower balance: VI = EI + I²REnergy Conservation CheckIf Lenz law were reversed:Induced current would AID fluxMore flux → more currentMore current → more fluxRunaway energy creation→ Violates energy conservationCorrect Lenz direction ensures:External work = electrical energyNo free energy possibleConservation enforced
Figure 2: Practical consequences of Lenz's law. Eddy current braking, motor back-emf regulation, and the thermodynamic argument for why the negative sign in Faraday's law is necessary.
  • Lenz's law is the direction law: induced current opposes the change in flux causing it. It is encoded in the negative sign of emf = -dΦ/dt.
  • Eddy current braking: induced currents in moving conductors oppose motion by the Lorentz force on the current-carrying conductor in the field.
  • Motor back-emf: a rotating motor generates a back-emf that opposes the applied voltage, limiting current. As motor speeds up, back-emf increases, reducing net current and torque until equilibrium.
  • Transformer loading: secondary current creates a flux opposing the primary flux. The primary must draw more current to maintain the core flux, which is how power is transferred.
  • The necessity of external work to change flux is the physical content of Lenz's law. Energy is always conserved in the process.

Quick Revision

  • Lenz's law: induced current direction always opposes the change in flux that caused it.
  • Mathematical form: contained in the negative sign of emf = -N·dΦ/dt.
  • Physical basis: conservation of energy. Aiding the change would create a self-sustaining runaway loop violating the first law of thermodynamics.
  • Direction method: (1) identify if flux increases or decreases, (2) find induced B direction to oppose change, (3) right-hand rule for current direction.
  • Applications: eddy current braking, back-emf in motors and generators, transformer coupling, metal detectors, induction heating.
  • Trap: Lenz's law gives direction only. Always use |emf| = N·|dΦ/dt| for magnitude, then apply Lenz for sign.
  • Lenz's law and Newton's third law analogy: both describe opposition or reaction to a cause, both enforce conservation (energy and momentum).

Lenz Law Applications

Test your grasp of Lenz's Law and its role in energy conservation during electromagnetic induction.

Question 1 of 3

Q1.Lenz's Law states that the direction of induced current in a loop is such that: