Objectives

Lesson outcomes

  • Explain that an e.m.f. is induced when a conductor cuts magnetic field lines or when the magnetic field linking a conductor changes.
  • State the factors that increase the size of the induced e.m.f.
  • Explain why the induced e.m.f. opposes the change that caused it.
  • Describe a simple a.c. generator and interpret an e.m.f.-time graph for one full rotation.
Syllabus

CIE 0625 syllabus points

7 linked

Definitions

Required definitions

  • Electromagnetic induction

    the process that produces a potential difference across a conductor due to relative movement between the conductor and a magnetic field.

Lesson Notes

Student guidance and lesson notes

Overview

This lesson introduces electromagnetic induction, which is one of the most important ideas in the topic. The key pattern is simple: if the magnetic field linking a conductor changes, an e.m.f. is induced. A generator is then just a device that keeps creating that change again and again.

What You Need to Know

  • An induced e.m.f. is produced when a conductor moves across a magnetic field or when the magnetic field linking the conductor changes.
  • You can demonstrate induction by moving a magnet into and out of a coil connected to a galvanometer.
  • A larger induced e.m.f. is produced by a stronger magnetic field, faster movement, or more turns in the coil.
  • The induced e.m.f. acts in a direction that opposes the change causing it. This is the key idea of Lenz’s law.
  • In a simple a.c. generator, a rotating coil in a magnetic field produces an alternating e.m.f.
  • Slip rings and brushes allow contact to be maintained while the coil rotates.
  • The e.m.f.-time graph rises to a peak, falls to zero, reaches a trough, and returns to zero over one full turn.

How to Work Through It

  1. Start with a magnet-and-coil demonstration so you can see induction happen before naming it.
  2. Identify which changes increase the size of the galvanometer deflection.
  3. Transfer the same idea to a rotating coil and label the parts of a simple a.c. generator.
  4. Match positions of the coil to the peaks, troughs, and zeros on the output graph.

Check Your Understanding

  • What must change for an e.m.f. to be induced?
  • How can you increase the size of the induced e.m.f.?
  • Why does the induced e.m.f. oppose the change that causes it?
  • At which coil positions is the generated e.m.f. zero and when is it greatest?

Common Mistakes

  • Thinking a stationary magnet near a coil always induces a current. There must be a change in the field linking the coil.
  • Mixing up split-ring commutators and slip rings. Generators use slip rings for alternating output.
  • Treating the graph as separate from the coil motion. Each peak and zero matches a specific coil position.

Next Steps

  • Use the slides and Lenz’s law questions to practise explaining induction with clear cause-and-effect language.
  • Keep the idea of alternating output secure because it feeds directly into the next lesson on transformers.
Lesson Resources

Materials for this lesson

Use these videos, slide decks, documents, or links to work through the lesson.

Document

Lenz's Law Practice

Questions to pratice applying Lenz's law

Open resource