Eduqas A-Level Physics A420QS
Basic Physics
Kinematics
Dynamics
Energy Concepts
Circular Motion
Vibrations
Kinetic Theory
Thermal Physics
Conduction of Electricity
Resistance
D.C. Circuits
Capacitance
Solids Under Stress
Electrostatic and Gravitational Fields of Force
Using Radiation to Investigate Stars
Orbits and the Wider Universe
The Nature of Waves
Wave Properties
Refraction of Light
Photons
Lasers
Nuclear Decay
Particles and Nuclear Structure
Nuclear Energy
Magnetic Fields
Electromagnetic Induction
Option A: Alternating CurrentsOption A
Option B: Medical PhysicsOption B
Option C: The Physics of SportsOption C
Option D: Energy and the EnvironmentOption D
Mathematical Requirements (Appendix C)
Option A: Alternating Currents
Electromagnetic induction in a rotating coil
- 3 things to know
- Component 3
Overview
Recall questions on why a coil turning at constant angular velocity produces a sinusoidal output rather than a steady one, the variation of flux linkage through the rotation, the quarter-cycle relationship between flux linkage and emf, and the effect of doubling the rotation rate.
What you need to know
Answer each one before you reveal it.
Give the equation for the emf induced in a flat coil rotating in a uniform B-field.
Why is the emf of a rotating coil zero twice in every revolution?
Questions from this subtopic
Each one with the model answer underneath.
- 1
Why does a coil rotating steadily in a uniform field generate a sinusoidal emf rather than a constant one?
Model answer
The rate at which the flux linkage changes varies through the rotation, reaching a maximum when the coil's plane lies along the field and zero a quarter turn later.
- 2
Why does a coil rotating steadily in a uniform magnetic field produce an emf at all?
Model answer
As the coil turns, the angle between its normal and the field changes continuously, so the flux linking the coil changes. A changing flux linkage induces an emf by Faraday's law.
- 3
Write down the expression for the flux linkage of a flat coil of N turns and area A rotating in a uniform field of flux density B.
Model answer
The flux linkage is NΦ = BAN cos ωt, in Wb turns. B is the flux density in T, A the coil area in m², N the number of turns and ω the angular velocity in rad s⁻¹.
- 4
Why can the angle between the coil normal and the field be written as ωt?
Model answer
The coil is driven at a steady angular velocity ω, so the angle it has turned through grows uniformly with time. Starting the clock when the normal is along the field makes that angle equal to ωt in radians.
- 5
At what orientation of the coil is the flux linkage a maximum, and what is its value there?
Model answer
The flux linkage is greatest when the coil normal lies along the field, so the plane of the coil is perpendicular to the field lines. Its value there is BAN in Wb turns.
- 6
At what orientation of the coil is the induced emf a maximum?
Model answer
The emf is greatest when the coil normal is perpendicular to the field, so the plane of the coil contains the field lines. At that instant the flux linkage is zero but it is changing at its fastest rate.
Other ways to work this
The same content, four other ways.
What is inside Levo
Six ways to work the same material.
Every question in Option A: Alternating Currents, on a schedule.
Attempt a question from memory, write the correct version, then attempt it again. Levo records the jump between your first attempt and your last, and brings each question back on the day you are due to forget it.
Or £46 a year, about £3.83 a month. Cancel anytime.