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12.2 Magnetism and Moving Charges

Part of Magnetic Fields and Electromagnetism in AP® Physics C: Electricity and Magnetism. Read the opening section, then create a free account for the full interactive lesson, practice, and progress tracking.

The magnetic force on a moving charge is given by the vector equation

FB=qv×B\mathbf{F}_B = q \mathbf{v} \times \mathbf{B}

Its magnitude is

FB=qvBsin⁡θF_B = qvB\sin\theta

where θ{\theta} is the angle between velocity and magnetic field. The right-hand rule gives the direction for a positive charge, and the force reverses for a negative charge. Since the force is perpendicular to both $mathbf{v}$ and B{\mathbf{B}}, a uniform magnetic field often produces circular motion when the velocity is perpendicular to the field.

If the motion is purely perpendicular, then the magnetic force serves as the centripetal force:

qvB=mv2rqvB = \frac{mv^2}{r}

which gives

r=mvqBr = \frac{mv}{qB}

and

T=2πmqBT = \frac{2\pi m}{qB}

Notice that the period does not depend on speed. This is one of the most elegant results in the unit and is the reason charged particles of fixed q/m cycle predictably in magnetic devices.

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