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SELF 
INDUCTANCE
•When an electric current is passed 
through an insulated conducting coil, it 
gives rise to a magnetic field in the coil 
so that the coil itself behaves like a 
magnet. 
•The magnetic flux produced by the 
current in the coil is linked with the coil 
itself.
DEFINATION 
As the strength of the current in the 
coil is changed, the flux linked with the coil 
also changes. Under such circumstances an 
emf is induced in the coil too. Such emf is 
called a self-induced emf and this 
phenomenon 
is known as self-induction.
Conducting coil 
Battery 
Direction of the Current 
Key/Switch Rheostat
Current flows 
In anti-clock 
Wise direction 
Current 
flows 
In clock 
Wise 
direction
If the number of turn in a coil is N and 
the flux linked with each turn is φ, then 
the total flux linked through the coil = 
Nφ. 
In this case, the total flux linked with 
the coil (which is called flux linkage) is 
directly proportional to the current I 
flowing through the coil.
N = LI 
where the constant of proportionality 
L is called the self-inductance of a coil. 
N = LI, L= N/I 
The self inductance L is a measure of 
the flux linked with coil per unit 
current.
•The self-inductance L of a coil depends 
upon – 
(1)The size and shape of the coil. 
(2) The number of turns N. 
(3) The magnetic property of the medium 
within the coil in which the flux exists. 
NOTE:Self-inductance L does not depend 
on current I.
Diffrentiating equation N = LI with 
respect to time t, 
N d/dt = L dI/dt 
In the case of self-induction, Faraday’s 
law and Lenz’s law holds good. Hence self-induced 
emf in the coil is, 
e = -N d/dt 
Self-induced emf is also called “back 
emf”.
Form equation e = -L dI/dt 
Self inductance L = -e/(dI/dt) 
“The self-induced emf produced per unit 
rate of change of current in the circuits 
called self-inductance of the circuit.” 
Unit of L =unit of emf(v)/Unit of rate 
of change of current (A/s)=Vs/A or 
Henry(H)
self inductance

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self inductance

  • 2. •When an electric current is passed through an insulated conducting coil, it gives rise to a magnetic field in the coil so that the coil itself behaves like a magnet. •The magnetic flux produced by the current in the coil is linked with the coil itself.
  • 3. DEFINATION As the strength of the current in the coil is changed, the flux linked with the coil also changes. Under such circumstances an emf is induced in the coil too. Such emf is called a self-induced emf and this phenomenon is known as self-induction.
  • 4. Conducting coil Battery Direction of the Current Key/Switch Rheostat
  • 5. Current flows In anti-clock Wise direction Current flows In clock Wise direction
  • 6. If the number of turn in a coil is N and the flux linked with each turn is φ, then the total flux linked through the coil = Nφ. In this case, the total flux linked with the coil (which is called flux linkage) is directly proportional to the current I flowing through the coil.
  • 7. N = LI where the constant of proportionality L is called the self-inductance of a coil. N = LI, L= N/I The self inductance L is a measure of the flux linked with coil per unit current.
  • 8. •The self-inductance L of a coil depends upon – (1)The size and shape of the coil. (2) The number of turns N. (3) The magnetic property of the medium within the coil in which the flux exists. NOTE:Self-inductance L does not depend on current I.
  • 9. Diffrentiating equation N = LI with respect to time t, N d/dt = L dI/dt In the case of self-induction, Faraday’s law and Lenz’s law holds good. Hence self-induced emf in the coil is, e = -N d/dt Self-induced emf is also called “back emf”.
  • 10. Form equation e = -L dI/dt Self inductance L = -e/(dI/dt) “The self-induced emf produced per unit rate of change of current in the circuits called self-inductance of the circuit.” Unit of L =unit of emf(v)/Unit of rate of change of current (A/s)=Vs/A or Henry(H)