It is convenient to express the induced emf in terms of the current in a circuit rather than the magnetic flux through it. If no magnetic materials are present, the magnetic field produced by a coil, and hence also the flux, are directly proportional to the current flowing through it,
Thus,Φ = L I
Where L is a constant of proportionality called the self-inductance of the coil. Its SI unit is henry (H). The self-inductance of a circuit depends on the size and shape.
Using Faraday's law the induced emf in the coil is given by
ε =
(4.11)
The polarity of the emf depends on the rate of change of the current, not on its magnitude or its direction. This is illustrated in Fig. 4.18.
Self-inductance of a solenoid
To a good approximation, the magnetic field inside the solenoid is uniform and given by
B = µ0
where n = N/ l is the number of turns per unit length, N the total number of turns, l the total length, and I the current in the solenoid.
The flux through the solenoid is
Φ = BNA = µ
0n
INA =
As expected, the flux is proportional to the current I. The proportionality constant is the
self-inductance.
L =
(4.12)
Example: 4.7
Find the self inductance of a solenoid of length 10 cm, area 5 cm2 and number of turns 100.
Solution
We know L =
Here µ0 = 4π × 10 -7 H/m; N = 100 ; A = 5 × 10 -4 m 2 ; l = 0.1 m
∴L =
= 2π × 10
-5
H