Introductory Physics Volume Two
Introductory Physics Volume Two
Introductory Physics Volume Two
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92 Magnetic Fields 4.6<br />
The net force is<br />
⃗F = îF 1 − ĵF 2<br />
= îIL 1 B − ĵIL 2 B<br />
So the direction is given by<br />
( ) ( )<br />
θ = tan −1 IL2 B<br />
= tan −1 L2<br />
,<br />
IL 1 B<br />
L 1<br />
where θ is below the x-axis. The magnitude of the force is<br />
√<br />
F =<br />
√F1 2 + F 2 2 = IB L 2 1 + L2 2<br />
Example<br />
What is the net force on an a × b rectangular loop of wire carrying a<br />
current I that is in a uniform magnetic field perpendicular to the loop’s<br />
plane?<br />
Assume a direction for the magnetic field and use the right hand rule<br />
to draw the forces on each segment of the loop:<br />
a<br />
F 1<br />
b<br />
F 2<br />
F 3<br />
F 4<br />
B<br />
The net force on the loop is:<br />
⃗F = ⃗ F 1 + ⃗ F 2 + ⃗ F 3 + ⃗ F 4<br />
= î(F 2 − F 4 ) + ĵ(F 3 − F 1 )<br />
= î(IbB − IbB) + ĵ(IaB − IaB)<br />
= 0<br />
I<br />
Example<br />
Show that the magnetic force due to a uniform magnetic field for any<br />
closed current loop is zero.<br />
The force law states<br />
∮<br />
⃗F = I d ⃗ l × B ⃗