Electromagnetic induction

When a coiled wire is introduced near a magnet, the magnetic lines of force pass through the coil. This causes the magnetic flux to change. Magnetic flux is represented by the symbol ${\displaystyle {\Phi }}$, therefore we can say that ${\displaystyle {\Phi }}$ = BAcos(a) and the resulting unit will be ${\displaystyle Tm^{2}}$, where T is the unit for magnetic field and ${\displaystyle m^{2}}$ is the unit for area.

The changing magnetic flux generates an electromotive force (EMF). This force moves free electrons in a certain way, which constitute a current.

Michael Faraday found that an electromotive force is generated when there is a change in magnetic flux in a conductor.

His laws state that:

${\displaystyle {\mathcal {E}}={-{d\Phi } \over dt}}$

where,

${\displaystyle {\mathcal {E}}}$ is the electromotive force, measured in volts;

${\displaystyle {d\Phi }}$ is the change in magnetic flux, measured in webers;

${\displaystyle dt}$ is the change in time, measured in seconds.

In the case of a solenoid:

${\displaystyle {\mathcal {E}}={-N{d\Phi } \over dt}}$

where,

N is the number of loops in the solenoid.

The negative sign in both equation above is a result of Lenz's law, named after Heinrich Lenz. His law states that the electromotive force (EMF) produces a current that opposes the motion of the changing magnetic flux.

• Electromagnetism
• Inductor
• Transformer