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Self Inductance, Mutual Inductance, and Energy Stored

Self inductance is the property of a coil by which a changing current in it induces an emf in the same coil. Mutual inductance is the property by which a changing current in one coil induces an emf in a nearby coil.

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Student-friendly explanation

In self induction, the coil's own changing current changes magnetic flux linked with it, producing back emf epsilon = -L dI/dt. In mutual induction, changing current in the primary coil changes flux linked with the secondary coil, producing induced emf epsilon = -M dI/dt. An inductor stores magnetic energy U = 1/2 L I^2.

How to write this in exams

  1. 1

    Start with the exact idea

    Self inductance is the property of a coil by which a changing current in it induces an emf in the same coil. Mutual inductance is the property by which a changing current in one coil induces an emf in a nearby coil.

  2. 2

    Then show how to use it

    Identify whether one coil or two coils are involved. Check whether current changes with time. Use L for same-coil induction and M for coupled coils. Calculate rate of change of current, then apply the emf formula with units. Use Lenz's law for sign or direction.

  3. 3

    Add one concrete example

    When current through an inductor is increased suddenly, the inductor opposes the rise of current by producing back emf. In a transformer-like pair of coils, changing current in one coil can induce emf in the other due to mutual inductance.

  4. 4

    Avoid this incomplete answer

    Applying epsilon = -L dI/dt when current is constant, or writing energy as LI^2 instead of 1/2 LI^2.

Definition

Self inductance is the property of a coil by which a changing current in it induces an emf in the same coil. Mutual inductance is the property by which a changing current in one coil induces an emf in a nearby coil.

Example

When current through an inductor is increased suddenly, the inductor opposes the rise of current by producing back emf. In a transformer-like pair of coils, changing current in one coil can induce emf in the other due to mutual inductance.

Rule to remember

Self induction: epsilon = -L dI/dt, where L is self inductance in henry, I is current in ampere, t is time in second, and epsilon is volt. Mutual induction: epsilon_2 = -M dI_1/dt, where M is mutual inductance in henry. Energy stored in an inductor: U = 1/2 L I^2 in joule. Use these when current changes with time, not for steady DC after transients settle.

Memory hook

Inductance reacts to change in current; no change means no induced back emf.

Examples and method

Worked example

An inductor of 0.80 H carries current increasing uniformly from 1.0 A to 3.0 A in 0.20 s. Magnitude of induced emf = L Delta I/Delta t = 0.80 x (2.0/0.20) = 8.0 V. Energy stored at 3.0 A is U = 1/2 L I^2 = 0.5 x 0.80 x 9.0 = 3.6 J. The induced emf opposes the increase of current.

Method to apply

Identify whether one coil or two coils are involved. Check whether current changes with time. Use L for same-coil induction and M for coupled coils. Calculate rate of change of current, then apply the emf formula with units. Use Lenz's law for sign or direction.

Diagram support

For self induction, show one coil with changing current and back emf. For mutual induction, show two nearby coils labelled primary and secondary, with changing current in the primary and induced emf in the secondary.

How CBSE asks it

Questions may ask definitions, SI unit henry, back emf reasoning, energy stored in an inductor, or comparison between self and mutual induction.

Avoid common mistakes

Common confusion

A common error is to treat inductance as resistance. Resistance opposes current itself, while inductance opposes change in current.

Common wrong answer

Applying epsilon = -L dI/dt when current is constant, or writing energy as LI^2 instead of 1/2 LI^2.

Exam tip

For self inductance, look for changing current in the same coil. For mutual inductance, look for two coils and changing current in one causing emf in the other.

Quick check

Why does an inductor oppose a sudden change in current?

An inductor opposes a sudden change in current because changing current changes magnetic flux linked with the coil, which induces a back emf. By Lenz's law, this induced emf acts against the change in current.

Answer writing and exam use

1-mark answer

Self inductance is the property of a coil by which a changing current in it induces an emf in the same coil. Mutual inductance is the property by which a changing current in one coil induces an emf in a nearby coil.

2-mark answer

Self inductance is the property of a coil by which a changing current in it induces an emf in the same coil. Mutual inductance is the property by which a changing current in one coil induces an emf in a nearby coil. Self induction: epsilon = -L dI/dt, where L is self inductance in henry, I is current in ampere, t is time in second, and epsilon is volt. Mutual induction: epsilon_2 = -M dI_1/dt, where M is mutual inductance in henry. Energy stored in an inductor: U = 1/2 L I^2 in joule. Use these when current changes with time, not for steady DC after transients settle. When current through an inductor is increased suddenly, the inductor opposes the rise of current by producing back emf. In a transformer-like pair of coils, changing current in one coil can induce emf in the other due to mutual inductance.

3-mark answer

In self induction, the coil's own changing current changes magnetic flux linked with it, producing back emf epsilon = -L dI/dt. In mutual induction, changing current in the primary coil changes flux linked with the secondary coil, producing induced emf epsilon = -M dI/dt. An inductor stores magnetic energy U = 1/2 L I^2. Self induction: epsilon = -L dI/dt, where L is self inductance in henry, I is current in ampere, t is time in second, and epsilon is volt. Mutual induction: epsilon_2 = -M dI_1/dt, where M is mutual inductance in henry. Energy stored in an inductor: U = 1/2 L I^2 in joule. Use these when current changes with time, not for steady DC after transients settle. An inductor of 0.80 H carries current increasing uniformly from 1.0 A to 3.0 A in 0.20 s. Magnitude of induced emf = L Delta I/Delta t = 0.80 x (2.0/0.20) = 8.0 V. Energy stored at 3.0 A is U = 1/2 L I^2 = 0.5 x 0.80 x 9.0 = 3.6 J. The induced emf opposes the increase of current. Questions may ask definitions, SI unit henry, back emf reasoning, energy stored in an inductor, or comparison between self and mutual induction. Applying epsilon = -L dI/dt when current is constant, or writing energy as LI^2 instead of 1/2 LI^2.
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