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Introductory Physics Volume Two

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4.2 Magnetic Force on a Current 81<br />

4 Magnetic Fields<br />

§ 4.1 Magnetic Field<br />

We have all played with magnets at some point. Magnets will<br />

attract some types of metals and can attract and repel other magnets.<br />

This seems similar to electric forces. Magnetic forces can indeed be<br />

explained in terms of magnetic fields, but the connection between the<br />

magnetic field and the magnetic force is significantly different from<br />

that for electric fields and force. The magnetic field is similar to the<br />

electric field in that they are both vector fields. We use the symbol B ⃗ to<br />

represent the magnetic field. If we put a compass needle in a magnetic<br />

field, the field will turn the needle until it is aligned with the direction<br />

of the field. At this point we will use the following simple operational<br />

definition of the magnetic field. The direction of the magnetic field<br />

is the direction that a compass needle points. The magnitude of the<br />

magnetic field is related to how strong the force is that aligns the needle<br />

with the direction of the field.<br />

A magnetic field does apply a force to charged particles. The<br />

magnetic force on the particle has the following properties:<br />

• F ∝ q<br />

• F ∝ v<br />

• F ∝ B<br />

• F ⃗ is perpendicular to both ⃗v and B. ⃗ These can be combined into the<br />

following succinct formula for the force.<br />

Fact: Magnetic Force<br />

A particle with charge q and velocity ⃗v in a magnetic field ⃗ B will<br />

feel a force<br />

⃗F = q ⃗v × ⃗ B<br />

Notice that there is no force if the velocity is parallel to the magnetic<br />

field. Also notice that the magnetic force is zero on a stationary<br />

particle.

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