Magnetic flux

Also called Phi_B

The amount of magnetic field passing through a surface, equal to the field magnitude times the area times the cosine of the angle between the field and the area vector. Measured in webers. Its change, not its size, is what drives induction.

The AP Physics 2 sheet prints it twice, as a dot product and as its expansion:

ΦB=BA=BcosθA\Phi_B = \vec{B} \cdot \vec{A} = \left|\vec{B}\right| \cos\theta \left|\vec{A}\right|

The unit is the weber, one tesla square metre. AP Physics C: Electricity and Magnetism generalises the same idea to a non-uniform field with ΦB=BdA\Phi_B = \int \vec{B} \cdot d\vec{A}, its topic 13.1.

The angle is the trap. θ\theta sits between the field and the area vector, which points perpendicular to the surface, not along it. A loop lying face-on to the field has θ=0\theta = 0 and maximum flux; turn it edge-on and θ=90\theta = 90 degrees puts the flux at zero even though the field never changed. Students who measure from the plane of the loop get every answer backwards.

Flux is a signed scalar, and the dot product supplies the sign: positive when the field runs along the area vector, negative when it runs against it. That sign is what makes "the flux is decreasing" a meaningful sentence rather than a comparison of magnitudes.

Nothing about a steady flux induces anything. Only ΔΦB/Δt\Delta \Phi_B / \Delta t appears in Faraday's law, and there are exactly three ways to change it: change BB, change the area AA, or rotate the loop to change θ\theta. Topic 12.4 works all three.

Back to the physics glossary