D.4.1 (HL)—Magnetic flux

Syllabus
First assessment 2025
Objective
Level
HL

Calculate Magnetic Flux

HL only

Define magnetic flux

Magnetic flux measures the magnetic field passing through an area. Here θ\theta is the angle between the field and the normal to the surface, not the surface itself. Flux has unit weber, Wb=Tm2\mathrm{Wb}=\mathrm{T\,m^2}.

\Phi=BA\cos\theta

Worked example — square loop

For side 6.2cm=6.2×102m6.2\,\mathrm{cm}=6.2\times10^{-2}\,\mathrm{m}, A=(6.2×102)2m2A=(6.2\times10^{-2})^2\,\mathrm{m^2}. In B=4.3×104TB=4.3\times10^{-4}\,\mathrm{T} with θ=45\theta=45^\circ, Φ=BAcosθ=1.2×106Wb\Phi=BA\cos\theta=1.2\times10^{-6}\,\mathrm{Wb}. For NN identical turns, flux linkage is NΦN\Phi.

Use flux linkage

For a coil with NN turns, the linked flux is NΦN\Phi. A change can result from changing BB, AA, θ\theta, or the number of turns. Keep the angle convention explicit: it is not generally the angle between B and the plane itself.

Check the geometry

At θ=0\theta=0, field and area normal align and Φ=BA\Phi=BA. At θ=90\theta=90^\circ, the field is parallel to the surface and Φ=0\Phi=0. Convert area to square metres before substitution.

Common trap

Do not use the angle between B and the plane when the formula expects the angle to the normal. Do not confuse flux Φ\Phi with flux linkage NΦN\Phi.

D.4.1 (HL) Exam Analysis

HL only

Assessment in practice

1 marks
How it is assessed

Questions identify flux through a coil at a stated orientation; the packet also contains one transformer item, which is adjacent but not direct evidence for flux frequency.

Command terms

State / What is

What earns marks

Use Φ=BA cosθ with θ measured from the area normal, include N only for flux linkage, and check limiting orientations.

Watch for

Using the plane angle instead of the normal angle, or adding a turn factor when the question asks for flux through one turn.

Representative question

Question 1

[Maximum number: 1]

State the magnetic flux linkage through the coil at t=0.

Retrieve the D.4 Induction Model

HL only

D.4 induction is secure when you connect geometry, rate of change and direction.

  • Magnetic flux: Φ=BA cosθ
  • Changing flux linkage induces emf by Faraday’s law
  • Motional emf: ε=BvL for a perpendicular moving conductor
  • Lenz’s law gives induced direction and reflects energy conservation
  • A rotating coil produces sinusoidal emf
  • Faster rotation shortens the period and increases peak emf when other variables are fixed