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Magnetic Flux and Magnetic Flux Density

 

This is part of the HSC Physics course under the topic Electromagnetic Induction.

HSC Physics Syllabus

  • describe how magnetic flux can change, with reference to the relationship `\phi =B_(||)A=BAcos\theta` (ACSPH083, ACSPH107, ACSPH109)

Magnetic Flux and Flux Density

This video explores what magnetic flux is and how it changes with reference to the relationship `\phi =B_(||)A=BAcos\theta`.

 

What is Magnetic Flux and Flux Density?

Magnetic flux is a measurement of the total number of magnetic field lines passing through a given area. Flux density is a measurement of the density of magnetic field lines. It is another name for the magnetic field strength `B`. So, Magnetic flux in a given area equals the flux density multiplied by the area.

Magnetic flux (in Webers, Wb) is given by:

  

$$\phi=B_{||}A=BA\cos{\theta}$$

 

where:

  • `B` is the magnetic field strength in Teslas (T) or Wb m–2.
  • `A` is the area of the conductor through which magnetic field lines project in metres squared (m2)
  • `\theta` is the angle between the magnetic field lines and the normal area of the area

 

 

From this equation, we deduce that:

  • when the surface is parallel to the magnetic field lines, its normal is perpendicular to the magnetic field (`\theta=90°`), thus the magnetic flux is zero.
  • when the surface is perpendicular to the magnetic field lines, its normal is parallel to the magnetic field (`\theta=0°`), thus the magnetic flux is maximum. 

Changes in Magnetic Flux

 

Any changes to the area, magnetic field strength and angle `\theta` results in a change in magnetic flux passing through the given area of a conductor.

 

 

For example, a change in magnetic flux occurs when the area moved to a location with differing magnetic flux, either higher or lower.

In the diagram above, a rectangular coil is moved out of a uniform magnetic field (directed into the page). As a result, the coil experiences a decrease in flux. 

  

 

Previous section: Interaction Between Two Parallel Current-carrying Conductors

Next section: Faraday's Law of Induction

 

RETURN TO MODULE 6: ELECTROMAGNETISM