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MAGNETIC FIELDS DUE TO CURRENTS

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PHY110W MAGNETISM <strong>MAGNETIC</strong> <strong>FIELDS</strong> <strong>DUE</strong> <strong>TO</strong> <strong>CURRENTS</strong><br />

FORCE BETWEEN<br />

TWO PARALLEL CONDUC<strong>TO</strong>RS<br />

d<br />

B L<br />

F a<br />

b<br />

ba<br />

F <br />

ab<br />

B <br />

a<br />

i a<br />

i b<br />

b<br />

The magnitude of the magnetic field due to the current<br />

in wire a at every point on wire b is given by<br />

B<br />

a<br />

µ 0ia<br />

=<br />

2π<br />

d<br />

and consequently the magnitude of the force on wire b<br />

due to the magnetic field of wire a (written F ba ) is<br />

µ 0Liaib<br />

Fba = iLB b a = = Fab<br />

(30-15)<br />

2π<br />

d<br />

• F ba and F ab are an action-reaction pair.<br />

• Parallel currents attract.<br />

• Antiparallel currents repel.<br />

The ampere can now be defined as …<br />

that unvarying current which, when maintained in each<br />

of two parallel conductors of infinite length and situated<br />

one metre apart in empty space, causes between them a<br />

force of exactly 2 × 10 -7 N per metre of length.<br />

19

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