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Inductance - Self Inductance

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Estimated time: 13 minutes
CBSE: Class 12
Maharashtra State Board: Class 11

Definition: Self-Inductance

The property of a coil by which it opposes the change in its own current and induces an emf in itself — numerically equal to the ratio of magnetic flux (produced due to current in the circuit) linked with the circuit to the current flowing in it, or the ratio of induced emf produced around the circuit to the rate of change of current in it — is called self-inductance.

OR

The self-inductance (L) of a coil is defined as the ratio of the total magnetic flux linkage through the coil to the current flowing in it. Equivalently, it equals the magnitude of the induced EMF per unit rate of change of current.

CBSE: Class 12

Formula: Self-Inductance

L = \[\frac{N\Phi_B}{I}\]

ε = -L\[\frac{dI}{dt}\]

Where:

Symbol Meaning SI Unit
L Self-inductance (coefficient) Henry (H)
N Number of turns in the coil
\[Φ_B\] Magnetic flux through one turn Weber (Wb)
I Current through the coil Ampere (A)
ε Induced EMF (self-induced) Volt (V)
dI/dt Rate of change of current A s⁻¹
CBSE: Class 12

SI Unit and Dimensional Formula

  • SI Unit: Henry (H) — named after Joseph Henry
  • 1 Henry = 1 Wb A⁻¹ = 1 V · s · A⁻¹ = 1 Ω · s
  • Dimensional Formula: [M L2 T−2 A−2]
CBSE: Class 12

Derivation: Self-Inductance of a Solenoid

Step 1: Set Up the Solenoid

Consider a long solenoid of:

  • Length: l
  • Cross-sectional area: A
  • Number of turns: N (total), with n = N/l turns per unit length
  • Current flowing: I
  • Core: Air (or vacuum), permeability μ0

Step 2: Find the Magnetic Field Inside

  • B = μ0 n I

Step 3: Find the Flux Linkage

Magnetic flux through one turn:

  • ΦB = B ⋅ A = μ0 n I A

Total flux linkage through all N turns:

  • B = N ⋅ μ0 n I A = μ0 n N I A

Since N = n l:

  • B = μ0 n2 I A l

Step 4: Apply the Definition

  • L = \[\frac{N\Phi_B}{I}=\frac{\mu_0n^2IAl}{I}\]
  • L = \[\mu_0n^2Al\]

Step 5: With a Magnetic Core (relative permeability μr​)

  • L = \[\mu_r\mu_0n^2Al\]
CBSE: Class 12

Energy Stored in an Inductor

When current builds up from 0 to I in an inductor, work is done against the back-EMF. This energy is stored as magnetic potential energy in the magnetic field:

W = \[\int_0^ILIdI=\frac{1}{2}LI^2\]

Comparison with Capacitor Energy:

Device Energy Stored Field
Inductor (L) \[\frac {1}{2}LI^2\] Magnetic
Capacitor (C) \[\frac {1}{2}CV^2\] Electric
CBSE: Class 12

Magnetic Energy Density

Energy stored per unit volume in the magnetic field of a solenoid:

uB = \[\frac {\text {W}}{\text{Volume}}\] = \[\frac{\frac{1}{2}LI^2}{Al}\]

Substituting L = μ0n2Al and B = μ0nI:

uB = \[{u_B = \frac{B^2}{2\mu_0}}\]
CBSE: Class 12

Self-Inductance vs. Mutual Inductance

Feature Self-Inductance (L) Mutual Inductance (M)
Definition EMF induced in the same coil EMF induced in a neighbouring coil
Formula L = NΦ/I M = \[N_2Φ_{21}/I_1\]
SI unit Henry (H) Henry (H)
Role Opposes a change in their current Couple two separate circuits
Application Choke coils, inductors Transformers, wireless charging
Sign of EMF Negative (Lenz's law) Depends on coil orientation
CBSE: Class 12

Example

The Question asks: Find the magnetic energy density inside a solenoid and compare it with the electric energy density.

What's happening step by step:

  1. Start with energy stored in the inductor:
    A solenoid with inductance L carrying current I stores energy:

    W = \[\frac {1}{2}\]LI2

  2. Substitute the solenoid formula L = μ0n2Al:

    W = \[\frac{1}{2}\mu_0n^2Al\cdot I^2\]
  3. Divide by volume (V = Al) to get energy per unit volume:

    uB = \[\frac{W}{Al}=\frac{1}{2}\mu_0n^2I^2\]
  4. Since B = μ0nI, substitute to simplify:

    uB = \[\frac {B^2}{2μ_0}\]

Shaalaa.com | Electromagnetic Induction Part 5

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Electromagnetic Induction Part 5 [00:48:23]
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