Q1. A coil of 500 turns experiences a flux change from 0.1 Wb to 0.4 Wb in 0.2 s. Find the induced EMF.
dΦ = 0.4 − 0.1 = 0.3 Wb
EMF = N dΦ/dt = 500 × 0.3 / 0.2
EMF = 750 V
Move a magnet near a coil and you make electricity. Learn the laws behind every generator and transformer, and compute the induced EMF.
Find the EMF induced in a rod moving perpendicular to a magnetic field (EMF = BLv).
The faster the rod moves (or the stronger the field), the larger the induced EMF — that is how a bicycle dynamo works.
Motional-EMF and flux-change problems with steps.
Loading…
Q1. A coil of 500 turns experiences a flux change from 0.1 Wb to 0.4 Wb in 0.2 s. Find the induced EMF.
dΦ = 0.4 − 0.1 = 0.3 Wb
EMF = N dΦ/dt = 500 × 0.3 / 0.2
EMF = 750 V
Q2. An aircraft with a wingspan of 20 m flies at 250 m/s where the vertical component of Earth's field is 5×10⁻⁵ T. Find the EMF across the wings.
EMF = B L v
EMF = 5×10⁻⁵ × 20 × 250
EMF = 0.25 V
| Quantity | Formula | SI unit |
|---|---|---|
| Magnetic flux | Φ = B A cosθ | weber (Wb) |
| Faraday's law | EMF = −N dΦ/dt | volt (V) |
| Motional EMF | EMF = B L v | V |
| Self-induced EMF | EMF = −L dI/dt | V |
| Energy in an inductor | U = ½ L I² | J |
The magnitude of the induced EMF in a circuit equals the rate of change of magnetic flux linked with it: EMF = −N·dΦ/dt.
The direction of an induced current is always such that it opposes the change in flux that caused it — a consequence of conservation of energy.
The EMF induced when a conductor of length L moves with velocity v across a magnetic field B: EMF = BLv.
Loops of induced current set up in a solid conductor by a changing magnetic field; they cause heating and are used in braking and induction heating.
Hi! Found an error or have a suggestion? Let us know and we'll fix it.
Thanks! Your feedback has been sent. We'll look into it.