Electromagnetic Induction
All magnets are surrounded by field lines that by definition are called lines of force and  run from the North pole to the South pole. Where these are close together ,the field is strong e.g. near to the poles. So we also need to  consider the area over which these field lines act.
Flux combines the strength of the magnetic field and the area through which the field lines pass. Flux  Φ  = BA sin  θ
There is more flux near the poles of a magnet than on the sides as there are more field lines in an area near the poles than in the same area on the side.
Example How much flux if a field of 5 Tesla acts at 35 º  to an area of 0.2 m² ?  Φ  = 5 x 0.2 x sin 35  = 0.574 Weber
If we move a magnet in a coil , the wires will be forced to cut field lines. This generates a force on the conductors in the wire. The conductors ( electrons ) will move, generating a current. We use Flemings right hand rule to find the direction of the current.
If we consider a coil of N turns , then we have N loops of wire. The magnetic flux linking the coil is called the  flux linkage  and is defined as  N Φ   This can be written as  BAN sin  θ
Faraday’s Law If a conductor passes through a magnetic field , the electrons will experience a force. If the conductor is not a complete circuit, an EMF will be produced across its ends. This EMF will depend on the rate at which the field lines are cut. E  d Φ dt
As the constant of proportionality is 1 , the equation becomes  E = -  d Φ dt For a coil of N turns  E =  - N d Φ dt  The minus sign is because it opposes the motion that created it.
Remember  B is  Flux Density measured in Tesla Φ  is flux measured in Weber

Electromagnetic Induction

  • 1.
  • 2.
    All magnets aresurrounded by field lines that by definition are called lines of force and run from the North pole to the South pole. Where these are close together ,the field is strong e.g. near to the poles. So we also need to consider the area over which these field lines act.
  • 3.
    Flux combines thestrength of the magnetic field and the area through which the field lines pass. Flux Φ = BA sin θ
  • 4.
    There is moreflux near the poles of a magnet than on the sides as there are more field lines in an area near the poles than in the same area on the side.
  • 5.
    Example How muchflux if a field of 5 Tesla acts at 35 º to an area of 0.2 m² ? Φ = 5 x 0.2 x sin 35 = 0.574 Weber
  • 6.
    If we movea magnet in a coil , the wires will be forced to cut field lines. This generates a force on the conductors in the wire. The conductors ( electrons ) will move, generating a current. We use Flemings right hand rule to find the direction of the current.
  • 7.
    If we considera coil of N turns , then we have N loops of wire. The magnetic flux linking the coil is called the flux linkage and is defined as N Φ This can be written as BAN sin θ
  • 8.
    Faraday’s Law Ifa conductor passes through a magnetic field , the electrons will experience a force. If the conductor is not a complete circuit, an EMF will be produced across its ends. This EMF will depend on the rate at which the field lines are cut. E d Φ dt
  • 9.
    As the constantof proportionality is 1 , the equation becomes E = - d Φ dt For a coil of N turns E = - N d Φ dt The minus sign is because it opposes the motion that created it.
  • 10.
    Remember Bis Flux Density measured in Tesla Φ is flux measured in Weber