20.5 Electromagnetic Induction


2026 Syllabus Objectives

By the end of this topic, you should be able to:

  1. Define magnetic flux as the product of the magnetic flux density and the cross-sectional area perpendicular to the direction of the magnetic flux density.
  2. Recall and use the formula Φ = BA.
  3. Understand and use the concept of magnetic flux linkage.
  4. Understand and explain experiments that demonstrate: that a changing magnetic flux can induce an e.m.f. in a circuit; that the induced e.m.f. opposes the change producing it; and the factors that affect the magnitude of the induced e.m.f.
  5. Recall and use Faraday's Law and Lenz's Law of electromagnetic induction.

What is Magnetic Flux?

Imagine a magnetic field made up of invisible lines flowing through space — we call these magnetic field lines. Now imagine holding a flat loop of wire in that field. Some of those field lines will pass through the area of the loop.

Magnetic flux (symbol: Φ, the Greek letter "phi") is a measure of how many magnetic field lines pass through a given area. More precisely:

Magnetic flux is defined as the product of the magnetic flux density and the cross-sectional area that is perpendicular (at right angles) to the direction of the magnetic field.

  • Magnetic flux density (symbol: B, unit: Tesla, T) is the strength of the magnetic field — how tightly packed the field lines are.
  • Cross-sectional area (symbol: A, unit: ) is the area of the surface the field lines are passing through.
  • Magnetic flux (symbol: Φ, unit: Weber, Wb) is the total "amount" of field passing through that area.

The Formula

Φ=BA\Phi = BA

SymbolQuantityUnit
ΦMagnetic fluxWeber (Wb)
BMagnetic flux densityTesla (T)
ACross-sectional area

Maximum and Minimum Flux

The amount of flux through an area depends on the angle between the field lines and the surface:

  • Maximum flux: when the field lines are perpendicular to the plane of the area (i.e., they pass straight through it at 90°). In this case, Φ = BA.
  • Minimum flux (zero): when the field lines are parallel to the plane of the area (i.e., they skim along the surface and don't pass through it at all). In this case, Φ = 0.

Think of it like rain falling on an umbrella. If you hold the umbrella flat (horizontal), all the rain hits it — maximum. If you tilt it completely sideways (vertical), no rain hits it — zero.

When the Field is at an Angle

If the magnetic field lines are not perfectly perpendicular to the area, you must take the component of B that is perpendicular. The formula becomes:

Φ=BAcosθ\Phi = BA\cos\theta

where θ is the angle between the magnetic field lines and the normal to the area (the normal is an imaginary line drawn at right angles to the surface).

  • When θ = 0°: cos 0° = 1, so Φ = BA (maximum — field is perpendicular to plane)
  • When θ = 90°: cos 90° = 0, so Φ = 0 (minimum — field is parallel to plane)

Examiner Tip: Be careful — θ is measured from the normal line (perpendicular to the surface), NOT from the surface itself. If a question tells you the angle between the field and the surface, subtract it from 90° to get θ.

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