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Relative motion between a conductor and a magnetic field
Induced emf = rate of change of magnetic flux linkage
Induced current opposes the change in magnetic flux
ε=NΔΦΔt\varepsilon = N \frac{\Delta \Phi}{\Delta t}ε=NΔtΔΦ
ε=Blv\varepsilon = Blvε=Blv
Number of turns in the coil
Falls slower due to opposing forces from induced currents
Conservation of energy
NΦ=BANcos(ωt)N\Phi = BAN\cos(\omega t)NΦ=BANcos(ωt)
ε=BANωsin(ωt)\varepsilon = BAN\omega\sin(\omega t)ε=BANωsin(ωt)
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