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Magnetic flux
If a single-turn coil of wire encloses an area A, and a magnetic field B makes an angle θ with the normal to the plane of the coil, the magnetic flux through the coil is given by Φ = AB cos θ.
Symbol for magnetic flux
Φ
Units for magnetic flux
Wb = Tm2
Flux linkage
If a coil consists of N turns, the flux linkage is given by NΦ
Symbol for flux linkage
NΦ
Units for flux linkage
Wb or Wb turn
Faraday’s law
When the flux linking an electrical circuit is changing, an emf is induced in the circuit of magnitude equal to the rate of change of flux linkage
E = − ∆(NΦ)/∆t
Lenz’s law
The direction of any current resulting from an induced emf is such as to oppose the change in flux linkage that is causing the current.
Fleming’s Right Hand Rule
Find the direction of the induced current

How to calculate induced emf
Calculate flux linkage at t=0 and flux linkage at t=t
Subtract one from the other
Divide by t
This gives the average emf induced over that time
2 ways to induce an emf
Changing area over time
Changing flux density over time
How to induce an emf by changing area over time
Increase area of loop —> flux linkage increases
Substitute area into equation for Faraday’s law
Calculate emf
How to induce an emf by changing flux density over time
Substitute into Faraday’s law
Divide by t
How induce an emf using a generator
Rotating coil in a magnetic field
Factors that affect instantaenous emf
Flux density
Area of coil
Angular velocity
Position of the coil
Explain how flux density affects instantaneous emf
Larger flux density
Larger flux linkage
In a given time, change in flux density would be larger
Induced emf would be greater
Explain how area of the coil affects instantaneous emf
Larger area
Larger flux linkage
Induced emf would be larger
Explain how angular velocity affects instantaneous emf
Larger angular velocity means the change in flux linkage would happen is a smaller time. Therefore, the induced emf would be larger but the frequency of the emf would also be larger.
Explain how the position of the coil affects instantaneous emf
At position A, the coil is vertical, therefore θ = 0° and cosθ = 1. The flux linkage is a maximum at that point; therefore, the rate of change of flux linkage is at its minimum. Emf = 0
At position B, the coil is vertical, therefore θ = 90° and cosθ = 0. The flux linkage is 0 at that point; therefore, the rate of change of flux linkage is at its maximum.
