10.2.3Magnetism and the Motor Effect
The Motor Effect — Edexcel GCSE Combined Science 1SC0 - Physics Revision Notes & Topical Questions
5 min read 9 parts Lesson 8 of 10
Part 1 of 7A force on a current in a field
When a wire carrying a current is placed in a magnetic field, the two fields interact and the wire experiences a force. This is the motor effect. It is the basis of electric motors, loudspeakers and many measuring instruments.
Why it happens
- the field of the wire, circles around it, adds to the external field on one side of the wire and subtracts on the other.
- The field is strengthened on one side and weakened on the other, and the wire is pushed from the strong-field side towards the weak-field side.
Part 2 of 7Conditions for the force
- The force is greatest when the wire is at right angles to the field and zero when it is parallel to the field lines.
- Fleming's left-hand rule (6.1.7) gives its direction.
Part 3 of 7Size of the force: F = BIl
For a straight wire at right angles to a uniform field:
F = B I l
where F is force in newtons (N), B is the magnetic flux density (field strength) in tesla (T), I is the current in amperes (A) and l is the length of wire in the field in metres (m).
The force increases if the current is increased, if the field is stronger (stronger magnets), or if a longer length of wire lies in the field. A coil with N turns experiences N times the force.
Part 4 of 7Reversing the force
The direction of the force reverses if either the current or the field is reversed. Reversing both leaves the force unchanged. This idea allows a motor to keep spinning in one direction (see the commutator below) and a loudspeaker cone to move back and forth when alternating current flows in its coil.
Part 5 of 7Demonstration: the catapult
A rigid copper rod rests across two horizontal rails between the poles of a strong horseshoe magnet. When a current flows through the rod it rolls along the rails. Reversing the current rolls it the other way; turning the magnet upside down also reverses the motion. A bigger current or a stronger magnet gives a greater acceleration.
Part 6 of 7Applications and the DC motor
In a simple motor, a rectangular coil sits between the poles of a magnet.
- so the forces on them are opposite,
- producing a turning effect (a moment) on the coil.
- and carbon brushes make contact with the rotating ring.
Explaining the force with fields
Imagine a wire carrying current into the page placed in a uniform field pointing to the right.
- so the total field is stronger; below the wire its field points to the left (opposite),
- so the total is weaker.
Worked reasoning about the direction
Think of a wire in a horizontal field from left to right with the current flowing away from you.
Part 7 of 7Worked examples
A wire of length 0.15 m, carrying 4.0 A, is at right angles to a uniform field of 0.30 T. Calculate the force.
F = BIl = 0.30 × 4.0 × 0.15 = 0.18 N.
A wire in a field of 0.050 T has a force of 0.020 N on a 0.20 m length when the current is I. Find I.
I = F / (Bl) = 0.020 / (0.050 × 0.20) = 2.0 A.
The current in a wire is doubled and the field halved. What happens to the force?
F ∝ BI, so F → (½)(2) = 1 times, the force stays the same.
Key terms
| Term | Meaning |
|---|---|
| Motor effect | Force on a current-carrying conductor in a magnetic field. |
| Flux density B | Measure of magnetic field strength, in tesla (T). |
| Commutator | Split ring that reverses current in a motor coil every half turn. |
| Brushes | Carbon contacts that touch the commutator. |
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