As stated in our previous introductory lesson on induced emf, Faraday's Law of Induction states
ε = -N(ΔΦ/Δt)
where
-
ε is the induced voltage in a coil, measured in volts
- N is the number of loops in the coil
-
Φ is the number of flux lines, Φ = BperpendicularA
- ΔΦ is the changing flux, measured in webers
- Δt is the time over which the change occurs, measured in seconds
When the number of flux lines is constant, no emf is induced in a coil. The number of flux lines can be changed in two ways:
- by changing the strength of the magnetic field OR
- by changing the area of the coil.
In this lesson we will investigate the second case when an emf is induced by changing a loop's cross-sectional area that is exposed to a constant external magnetic field. This is called motional emf.
The following physlets show two ways of changing the coil's area and the resulting induced emf:
Sample Problem
In the following diagram, suppose that the green cross bar is moving to the right at a constant velocity, v. As it moves, the area of the "loop" presented to the magnetic field (+z) increases consequently allowing more flux lines to pass through the "loop" and generating an emf in the "loop."
ε = -N(ΔΦ/Δt)
ε = -N (BperpendicularΔA) /Δt
ε = -NB perpendicular (  Δw) /Δt
ε = -NB perpendicular (Δw/Δt)
ε = -NB perpendicular v
and obeys the formula
motional ε = - NB perpendicularv 
The right-hand curl rule is used to determine the direction of the induced emf/current. In this formula, v is the constant velocity in m/sec with which the loop is moving into or out of the magnetic field and  is the length of the side of the loop which does not change.
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We will now look at these two AP essays to verify that you understand the principles of induced emf.