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United StatesPhysics C: Electricity and MagnetismSyllabus dot point

How does a magnetic field exert a force on a moving charge or a current-carrying wire?

Topic 12.2 Magnetism and Moving Charges: apply the magnetic force on moving charges and currents, including circular motion and the force on a wire.

A calculus-based answer to AP Physics C E&M Topic 12.2, covering the magnetic force on a moving charge, the right-hand rule, circular motion in a field, the force on a current-carrying wire, and combined electric and magnetic forces.

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  1. What this topic is asking
  2. The magnetic force on a moving charge
  3. No work, so circular motion
  4. Force on a current-carrying wire
  5. Try this

What this topic is asking

The College Board (Topic 12.2) wants you to apply the magnetic force on a moving charge, F=qv×B\vec{F} = q\vec{v}\times\vec{B}, use the right-hand rule, analyze the circular motion of a charge in a uniform field, and find the force on a current-carrying wire, F=IL×B\vec{F} = I\vec{L}\times\vec{B}.

The magnetic force on a moving charge

The cross product makes the force perpendicular to both the velocity and the field. Point the right hand's fingers along v\vec{v}, curl toward B\vec{B}; the thumb gives v×B\vec{v}\times\vec{B} (reverse it for a negative charge). A charge moving along the field feels no force.

No work, so circular motion

Because Fv\vec{F}\perp\vec{v} always, the magnetic force does no work: Fv=0\vec{F}\cdot\vec{v} = 0. The speed and kinetic energy stay constant; only the direction turns. For a charge moving perpendicular to a uniform field, this perpendicular force is exactly centripetal, producing uniform circular motion. Setting the magnetic force equal to mv2r\dfrac{mv^2}{r}:

qvB=mv2rr=mvqB,T=2πmqBqvB = \frac{mv^2}{r} \quad\Longrightarrow\quad r = \frac{mv}{qB}, \qquad T = \frac{2\pi m}{qB}

The period is independent of speed (the basis of the cyclotron). If the velocity also has a component along B\vec{B}, the path becomes a helix.

Force on a current-carrying wire

A wire carrying current II is a stream of moving charges, so it feels a magnetic force:

F=IL×B,F=BILsinθ\vec{F} = I\vec{L}\times\vec{B}, \qquad F = BIL\sin\theta

where L\vec{L} points along the wire in the current's direction and θ\theta is the angle between the wire and the field. This is how motors generate torque.

Try this

Q1. A charge moves parallel to a magnetic field. State the magnetic force on it. [1 point]

  • Cue. Zero: F=qvBsinθF = qvB\sin\theta with θ=0\theta = 0.

Q2. An electron moves at 3.0×1063.0\times10^6 m/s perpendicular to a 0.200.20 T field. Find the force magnitude. [2 points]

  • Cue. F=qvB=(1.6×1019)(3.0×106)(0.20)=9.6×1014F = qvB = (1.6\times10^{-19})(3.0\times10^6)(0.20) = 9.6\times10^{-14} N.

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 2022 (style)1 marksSection I (multiple choice). A charged particle moves through a uniform magnetic field. The magnetic force on it does work on the particle equal to (A) qvBqvB (B) qvBsinθqvB\sin\theta (C) zero (D) 12mv2\tfrac{1}{2}mv^2. Justify your reasoning.
Show worked answer →

A 1-point MCQ on the work done by the magnetic force. The answer is (C).

The magnetic force F=qv×B\vec{F} = q\vec{v}\times\vec{B} is always perpendicular to the velocity, so Fv=0\vec{F}\cdot\vec{v} = 0 and the work is zero. The field changes the particle's direction but never its speed or kinetic energy. The trap is (A): that is the maximum force magnitude, not the work.

AP 2024 (style)5 marksSection II (FRQ, quantitative). A proton (charge +e+e, mass 1.67×10271.67\times10^{-27} kg) moves at 2.0×1062.0\times10^6 m/s perpendicular to a uniform 0.500.50 T field. (a) Calculate the magnetic force magnitude. (b) Explain the resulting path. (c) Calculate the radius of the path.
Show worked answer →

A 5-point FRQ on circular motion in a magnetic field.

(a) Force (2 points): F=qvBsin90=(1.6×1019)(2.0×106)(0.50)=1.6×1013F = qvB\sin 90^\circ = (1.6\times10^{-19})(2.0\times10^6)(0.50) = 1.6\times10^{-13} N.
(b) Path (1 point): the force is always perpendicular to the velocity, so it is centripetal: the proton moves in a circle at constant speed.
(c) Radius (2 points): the magnetic force provides the centripetal force, qvB=mv2rqvB = \dfrac{mv^2}{r}, so r=mvqB=(1.67×1027)(2.0×106)(1.6×1019)(0.50)=4.2×102r = \dfrac{mv}{qB} = \dfrac{(1.67\times10^{-27})(2.0\times10^6)}{(1.6\times10^{-19})(0.50)} = 4.2\times10^{-2} m.

Markers reward the force, the centripetal reasoning, and r=mv/qBr = mv/qB.

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