AcademyElectromagnetic Induction

Academy

Faraday's Law

Level 1 - Physics topic page in Electromagnetic Induction.

Principle

Faraday's law makes induced emf equal to the negative rate of change of magnetic flux linkage.

Notation

\(\mathcal E\)
induced emf
\(\mathrm{V}\)
\(N\)
number of turns in the coil
1
\(\Phi_B\)
magnetic flux through one turn
\(\mathrm{Wb}\)
\(B\)
uniform magnetic field magnitude
\(\mathrm{T}\)
\(A\)
loop area
\(\mathrm{m^{2}}\)
\(\theta\)
angle between field and area normal
\(\mathrm{rad}\)

Method

Derivation 1: Flux linkage

A coil with \(N\) identical turns links the same flux through each turn.

One-turn flux
\[\Phi_B=\int\vec B\cdot d\vec A\]
Flux linkage
\[N\Phi_B\]

Derivation 2: Faraday's law

The induced emf depends on how fast the flux linkage changes. The minus sign encodes the opposition direction.

Induction law
\[\mathcal E=-\frac{d}{dt}(N\Phi_B)\]
Constant turns
\[\mathcal E=-N\frac{d\Phi_B}{dt}\]
Magnitude
\[|\mathcal E|=N\left|\frac{d\Phi_B}{dt}\right|\]

Derivation 3: Uniform-field loop

If \(B\), \(A\), or \(\theta\) changes, differentiate \(BA\cos\theta\) with respect to time.

Uniform flux
\[\Phi_B=BA\cos\theta\]
Changing field only
\[\mathcal E=-NA\cos\theta\frac{dB}{dt}\]
Changing area only
\[\mathcal E=-NB\cos\theta\frac{dA}{dt}\]

Rules

These are the working forms of Faraday's law.

Faraday's law
\[\mathcal E=-N\frac{d\Phi_B}{dt}\]
Magnitude
\[|\mathcal E|=N\left|\frac{\Delta\Phi_B}{\Delta t}\right|\]
Uniform flux
\[\Phi_B=BA\cos\theta\]
Changing field
\[\mathcal E=-NA\cos\theta\frac{dB}{dt}\]

Examples

Question
A
\[30\]
-turn coil has flux per turn changing from
\[0.020,mathrm{Wb}\]
to
\[0.005,mathrm{Wb}\]
in
\[0.10,mathrm{s}\]
Find
\[|mathcal E|\]
Answer
[|mathcal E|=Nleft| rac{DeltaPhi_B}{Delta t} ight|=30 rac{|0.005-0.020|}{0.10}=4.5,mathrm{V}]

Checks

  • Use flux per turn with the factor \(N\), not total area unless the turns are distinct surfaces.
  • The minus sign gives direction; magnitudes use absolute values.
  • Flux is in webers, and \(1\,\mathrm{Wb\,s^{-1}}=1\,\mathrm{V}\).
  • If \(B\), \(A\), and \(\theta\) are all constant, \(\mathcal E=0\).