Self Inductance of a Current Carrying Solenoid: Consider a solenoid of radius r metre, length l metre, having total number of turns N and carrying a current I ampere. The magnetic field produced on its axis inside the solenoid is
B=μ0NIlNA−1m−1
If it is assumed that the solenoid is very long, the intensity of magnetic field B can be assumed to be uniform inside it at each point, then the total magnetic flux linked with the solenoid is
B=μ0m4π⎡⎢
⎢⎣d2+l2+2dl−(d2+l2−2dl){(d−l)(d+l)}2⎤⎥
⎥⎦
ϕ=B× total effective area of solenoid
=B×(NA)
where A=πr2 is the area of cross section of solenoid.
∴ϕ=μ0NIl×NA=μ0N2AIl weber
But by definition ϕ=LI where L is the self-inductance of solenoid, therefore
Self inductance L=ϕI=μ0N2Al henry
If inside the solenoid instead of air or vacuum there is a substance of relative permeability
L=μ0μrN2Al henry
Thus, the self inductance of a solenoid depends on the following factors:
(i) On the number of turns in the solenoid: The self inductance increases on increasing the number of turns.
(ii) On the area of cross section of solenoid (i.e., on the radius of solenoid): The self inductance increases on increasing the area of cross section.
(iii) On the length of solenoid: On increasing the length of solenoid, its self inductance decreases.
(iv) On the relative permeability of the substance placed inside the solenoid: If a soft iron rod is placed inside the solenoid, its self inductance increases.
Remember that if the number of turns per unit length in the solenoid is n, then n=N/l and the self inductance of solenoid is
L=μ0n2lA henry.