What is magnetic flux, and how is it computed as a surface integral of the field?
Topic 13.1 Magnetic Flux: define magnetic flux as the surface integral of the field and compute it for uniform and changing configurations.
A calculus-based answer to AP Physics C E&M Topic 13.1, covering magnetic flux as the surface integral of B, the area vector and angle dependence, flux through a coil of N turns, and how flux changes with field, area or orientation.
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What this topic is asking
The College Board (Topic 13.1) wants you to define magnetic flux as the surface integral of the field through a loop, compute it for uniform and angled configurations, and recognize the three ways it can change. Magnetic flux is the quantity whose rate of change drives induction in the rest of the unit.
Defining magnetic flux
The dot product means only the component of along the surface normal threads the surface. A field skimming parallel to the surface produces no flux; a field perpendicular to it produces the maximum, . When the field is non-uniform or the surface is curved, the flux is the genuine surface integral , summing over every patch. For the loops in this course the field is usually uniform across a flat area, so the simple form applies, but the integral definition is what makes magnetic flux the same kind of quantity as the electric flux of Unit 8.
The angle and the area vector
The angle is measured between and the surface normal, not the surface itself. A common slip is to use the field's angle with the plane of the loop; the two differ by . When the loop's plane faces the field (normal parallel to ), and ; when the plane lies along the field (normal perpendicular to ), and .
Flux linkage and the three ways flux changes
For a coil of identical turns, the total flux linkage is , which is what matters for induction: each turn contributes the same flux, so a coil of many turns multiplies the effect, which is why generators and transformers use coils of hundreds of turns. The flux can change in exactly three ways:
- the field changes (for example a magnet moves closer),
- the area enclosed changes (a loop is stretched or a bar slides),
- the orientation changes (the loop rotates, as in a generator).
Try this
Q1. A T field passes perpendicularly through a m squared loop. Find the flux. [1 point]
- Cue. Wb.
Q2. List the three ways the flux through a loop can change. [1 point]
- Cue. Change the field , the area , or the orientation angle .
Exam-style practice questions
Practice questions written in the style of College Board exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.
AP 2021 (style)1 marksSection I (multiple choice). A flat coil of area sits in a uniform field with its plane perpendicular to the field. The coil is then rotated so its plane is parallel to the field. The magnetic flux changes from (A) to zero (B) zero to (C) to (D) to . Justify your reasoning.Show worked answer →
A 1-point MCQ on the orientation dependence of flux. The answer is (A).
Flux is , with between and the area vector (the normal). When the plane is perpendicular to , the normal is parallel to (, ). When the plane is parallel to , the normal is perpendicular to (, ). The trap is confusing the plane's orientation with the normal's.
AP 2024 (style)4 marksSection II (FRQ, quantitative). A circular coil of turns and radius m sits in a uniform T field. (a) Calculate the flux through one turn when the coil's plane is perpendicular to the field. (b) Calculate the total flux linkage through all turns. (c) State what happens to the flux if the field is halved.Show worked answer →
A 4-point FRQ on flux through a multi-turn coil.
(a) Single-turn flux (2 points): area m squared. With the plane perpendicular to , : Wb.
(b) Flux linkage (1 point): Wb.
(c) Halving the field (1 point): flux is proportional to , so halving the field halves the flux.
Markers reward the single-turn flux, the linkage, and the proportionality to .
Related dot points
- Topic 13.2 Electromagnetic Induction: apply Faraday's law and Lenz's law to find the magnitude and direction of an induced EMF.
A calculus-based answer to AP Physics C E&M Topic 13.2, covering Faraday's law of induction, the rate of change of flux, Lenz's law for direction, motional EMF, and induced EMF in rotating coils.
- Topic 13.3 Induced Currents and Magnetic Forces: analyze the forces on induced currents, the energy and power in induction, and eddy-current effects.
A calculus-based answer to AP Physics C E&M Topic 13.3, covering the force on an induced current, the energy balance of a sliding rod, the power dissipated, eddy currents and magnetic braking.
- Topic 13.4 Inductance: define self-inductance, find the inductance and stored energy of a solenoid, and apply the back-EMF of an inductor.
A calculus-based answer to AP Physics C E&M Topic 13.4, covering self-inductance, the back-EMF, the inductance of a solenoid, the energy stored in an inductor, and the magnetic energy density.
- Topic 12.1 Magnetic Fields: describe magnetic fields, their sources in moving charges and magnets, field-line representation, and the absence of magnetic monopoles.
A calculus-based answer to AP Physics C E&M Topic 12.1, covering the magnetic field, its sources in moving charge, dipoles and field lines, Gauss's law for magnetism, and how magnetic fields differ from electric fields.
- Topic 8.5 Electric Flux: define electric flux as the surface integral of the field and compute it for uniform and non-uniform fields through flat and closed surfaces.
A calculus-based answer to AP Physics C E&M Topic 8.5, covering the area vector, the dot product, the flux surface integral, uniform-field and angle-dependent flux, and the net flux through a closed surface.
Sources & how we know this
- AP Physics C: Electricity and Magnetism Course and Exam Description — College Board (2024)