Inductance and Energy Storage

サイト: Young Education
コース: Induction
ブック: Inductance and Energy Storage
印刷者: Guest user
日付: 2026年 11月 9日(月曜日) 16:39

1. Inductance in Solenoids

Learning outcomes
  • I can define inductance.
  • I can explain how solenoids behave as inductors.
  • I can identify factors affecting inductance.
  • I can describe how coil geometry influences inductance.
  • I can solve simple inductance problems.

Inductance in Solenoids

Inductance is the ability of a conductor or circuit to produce an induced EMF when the current through it changes.

A coil of wire has much greater inductance than a straight wire because the magnetic fields produced by its individual turns reinforce one another. A long coil containing many closely spaced turns is called a solenoid.

Solenoids are therefore natural inductors.

When current through a solenoid changes:

changing current → changing magnetic field → changing magnetic flux → self-induced EMF

The self-induced EMF acts to oppose the change in current according to Lenz's law.

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6

What Is Inductance?

Inductance measures how strongly a circuit responds to a changing current by producing a self-induced EMF.

The symbol for inductance is:

L

The SI unit is the:

henry (H)

The relationship between induced EMF and changing current is:

ε = −L ΔI/Δt

where:

  • ε = self-induced EMF in volts (V)
  • L = inductance in henries (H)
  • ΔI = change in current in amperes (A)
  • Δt = time interval in seconds (s)

For magnitude calculations:

|ε| = L|ΔI/Δt|


Meaning of One Henry

A circuit has an inductance of:

1 H

if a current changing at:

1 A/s

produces an induced EMF with magnitude:

1 V

Therefore:

1 H = 1 V·s/A

Large inductance means a given rate of current change produces a relatively large self-induced EMF.


Why a Solenoid Has Inductance

A solenoid consists of many turns of wire.

When current flows through each turn, it produces a magnetic field.

Inside the solenoid, the fields from the individual turns combine.

This creates a relatively strong magnetic field along the solenoid's axis.

When the current changes, this magnetic field changes.

The changing field changes the magnetic flux through the turns of the solenoid.

Faraday's law then produces a self-induced EMF.


Magnetic Field Inside a Solenoid

For an ideal long solenoid:

B = μNI/l

where:

  • B = magnetic field strength
  • μ = magnetic permeability of the material inside the solenoid
  • N = number of turns
  • I = current
  • l = length of the solenoid

The quantity:

N/l

represents the number of turns per unit length.

The equation shows that the magnetic field becomes stronger when:

  • current increases
  • number of turns increases
  • magnetic permeability increases

For the ideal model, increasing the solenoid length while keeping N and I fixed spreads the turns farther apart and decreases the field.

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7

Magnetic Flux Through a Turn

Magnetic flux through one turn can be written:

Φ = BA

when the magnetic field is perpendicular to the area of the loop.

For a solenoid:

B = μNI/l

Therefore:

Φ = (μNI/l)A

or:

Φ = μNIA/l

The flux through each turn depends on:

  • current
  • number of turns
  • cross-sectional area
  • solenoid length
  • magnetic permeability

Flux Linkage

A solenoid contains many turns.

If the magnetic flux through one turn is Φ, the total flux linkage is:

NΦ

Substituting the expression for flux:

NΦ = N(μNIA/l)

Therefore:

NΦ = μN²AI/l

Inductance can be defined using flux linkage:

L = NΦ/I

Substituting:

L = μN²A/l

This is the important inductance equation for an ideal long solenoid.


Inductance Equation for a Solenoid

For an ideal long solenoid:

L = μN²A/l

where:

  • L = inductance in henries (H)
  • μ = magnetic permeability in H/m
  • N = number of turns
  • A = cross-sectional area in m²
  • l = length of the solenoid in m

This equation reveals how the geometry and material of a solenoid affect its inductance.


Factors Affecting Inductance

The inductance of an ideal solenoid depends mainly on:

  • number of turns, N
  • cross-sectional area, A
  • solenoid length, l
  • magnetic permeability, μ

The relationship is:

L = μN²A/l

Therefore:

L ∝ N²

L ∝ A

L ∝ μ

L ∝ 1/l

These relationships are extremely useful for comparing solenoids without doing a complete calculation.


Effect of Number of Turns

Inductance is proportional to the square of the number of turns:

L ∝ N²

This means that changing the number of turns has a particularly large effect.

If N doubles:

N → 2N

then:

L → (2²)L

Therefore:

L becomes 4 times larger

If N triples:

L becomes 9 times larger

This is one of the most important relationships for solenoids.


Why the Number of Turns Is Squared

The N² relationship occurs for two reasons.

First, increasing N increases the magnetic field:

B ∝ N

Second, increasing N also increases the number of turns linked by that magnetic flux.

Therefore:

one factor of N strengthens the field

and:

another factor of N increases flux linkage

Together:

L ∝ N²


Example: Changing the Number of Turns

Solenoid A has inductance:

L₁ = 0.20 H

Its number of turns is doubled while all other properties remain unchanged.

Since:

L ∝ N²

then:

L₂/L₁ = (N₂/N₁)²

L₂/L₁ = 2²

L₂ = 4(0.20)

L₂ = 0.80 H


Effect of Cross-Sectional Area

Inductance is directly proportional to cross-sectional area:

L ∝ A

A larger cross-sectional area allows more magnetic flux to pass through each turn.

Therefore:

larger area → greater flux linkage → greater inductance

If the area doubles while everything else remains unchanged:

inductance doubles


Diameter and Area

For a circular solenoid:

A = πr²

Therefore, changing the radius has a squared effect on area.

Suppose the radius doubles:

r → 2r

Then:

A → π(2r)²

A → 4πr²

Therefore:

area becomes 4 times larger

and, if all other factors remain constant:

inductance becomes 4 times larger


Example: Changing Radius

A solenoid has inductance:

L₁ = 0.15 H

Its radius is doubled while all other factors remain unchanged.

Because:

A ∝ r²

the area becomes four times larger.

Since:

L ∝ A

the new inductance is:

L₂ = 4(0.15)

L₂ = 0.60 H


Effect of Solenoid Length

For an ideal solenoid with a fixed number of turns:

L ∝ 1/l

Therefore, increasing the length reduces inductance.

If the solenoid length doubles while N, A, and μ remain constant:

inductance becomes half as large

This occurs because the turns become more spread out, weakening the magnetic field.


Important Condition About Length

The statement:

L ∝ 1/l

assumes that the number of turns remains constant.

If a longer solenoid is made by adding additional turns while keeping the same turns per metre, both N and l change.

The effect must then be analyzed using the full equation:

L = μN²A/l

Always check which quantities are being held constant.


Example: Changing Length

A solenoid has:

L₁ = 0.40 H

Its length is doubled while the number of turns, area, and core material remain unchanged.

Since:

L ∝ 1/l

then:

L₂ = L₁/2

L₂ = 0.20 H


Effect of Core Material

The magnetic permeability μ describes how a material responds to a magnetic field.

For an air-core solenoid:

μ ≈ μ₀

where:

μ₀ = 4π × 10⁻⁷ H/m

Placing a suitable magnetic material inside the solenoid can greatly increase the magnetic field and flux.

Therefore:

higher permeability → greater inductance

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5

Relative Permeability

For many materials:

μ = μ₀μᵣ

where:

  • μ₀ = permeability of free space
  • μᵣ = relative permeability of the material

For air:

μᵣ ≈ 1

Some magnetic materials have much larger relative permeabilities.

Using such a core can therefore greatly increase inductance.

In real materials, however, permeability may depend on field strength, frequency, temperature, and other factors.


Air-Core Solenoids

An air-core solenoid contains no strongly magnetic core material.

Advantages can include:

  • predictable inductance
  • no magnetic-core saturation
  • useful behaviour at high frequencies

However, its inductance may be smaller than that of a similar coil containing a high-permeability magnetic core.


Magnetic-Core Solenoids

Adding a suitable magnetic core can concentrate the magnetic field.

This increases:

  • magnetic flux
  • flux linkage
  • inductance

Magnetic cores are therefore widely used in inductors and transformers.

Different applications use different core materials depending on the required frequency, inductance, efficiency, and power.


Coil Geometry

The geometry of a coil determines how effectively its magnetic field links its turns.

For a long ideal solenoid, the most important geometrical quantities are:

  • number of turns
  • length
  • cross-sectional area

A coil with:

  • many turns
  • a large cross-sectional area
  • relatively short length

will generally have greater inductance than one with:

  • few turns
  • small area
  • greater length

assuming the same core material.


Comparing Two Solenoids

Suppose two air-core solenoids have the same length and cross-sectional area.

Solenoid A:

N = 200 turns

Solenoid B:

N = 400 turns

Since:

L ∝ N²

then:

L_B/L_A = (400/200)²

L_B/L_A = 2²

L_B/L_A = 4

Solenoid B has four times the inductance.


Worked Example: Air-Core Solenoid

An air-core solenoid has:

N = 1000 turns

A = 2.0 × 10⁻⁴ m²

l = 0.50 m

Use:

L = μ₀N²A/l

with:

μ₀ = 4π × 10⁻⁷ H/m

Substitute:

L = (4π × 10⁻⁷)(1000²)(2.0 × 10⁻⁴)/(0.50)

First:

1000² = 1.0 × 10⁶

Therefore:

L ≈ 5.0 × 10⁻⁴ H

So:

L ≈ 0.00050 H

or:

L ≈ 0.50 mH


Millihenries and Microhenries

Many practical inductors have values much smaller than one henry.

Useful units include:

1 mH = 10⁻³ H

and:

1 μH = 10⁻⁶ H

For example:

0.005 H = 5 mH

0.000020 H = 20 μH

Being comfortable converting between these units is important in inductance calculations.


Worked Example: Magnetic-Core Solenoid

A solenoid has:

N = 500

A = 4.0 × 10⁻⁴ m²

l = 0.20 m

The core has permeability:

μ = 2.0 × 10⁻⁴ H/m

Use:

L = μN²A/l

L = (2.0 × 10⁻⁴)(500²)(4.0 × 10⁻⁴)/(0.20)

Since:

500² = 250,000

then:

L = 0.10 H

Therefore:

L = 0.10 H


Worked Example: Finding the Number of Turns

A solenoid has:

L = 0.080 H

A = 5.0 × 10⁻⁴ m²

l = 0.25 m

μ = 1.0 × 10⁻⁴ H/m

Start with:

L = μN²A/l

Rearrange:

N² = Ll/(μA)

Substitute:

N² = (0.080)(0.25)/[(1.0 × 10⁻⁴)(5.0 × 10⁻⁴)]

N² = 400,000

Therefore:

N = √400,000

N ≈ 632 turns

A real coil would use a whole number of turns, so approximately 632 turns would be required under the ideal assumptions.


Worked Example: Finding Cross-Sectional Area

A solenoid has:

L = 0.050 H

N = 800

l = 0.40 m

μ = 1.0 × 10⁻⁴ H/m

Use:

L = μN²A/l

Rearrange:

A = Ll/(μN²)

Substitute:

A = (0.050)(0.40)/[(1.0 × 10⁻⁴)(800²)]

A = 0.020/64

A = 3.125 × 10⁻⁴ m²

Approximately:

A = 3.1 × 10⁻⁴ m²


Inductance and Induced EMF

Once the inductance is known, the induced EMF can be calculated using:

|ε| = L|ΔI/Δt|

Suppose:

L = 0.40 H

and the current changes from:

1.0 A to 5.0 A

in:

0.20 s

Then:

ΔI = 4.0 A

and:

ΔI/Δt = 20 A/s

Therefore:

|ε| = (0.40)(20)

|ε| = 8.0 V

The induced EMF acts to oppose the change in current.


Combining the Ideas

The two important equations are:

L = μN²A/l

and:

|ε| = L|ΔI/Δt|

Together they show how the physical construction of a solenoid affects its electrical behaviour.

For example:

more turns → greater L → greater self-induced EMF for the same rate of current change

Similarly:

larger area → greater L → greater self-induced EMF


Inductance and Energy Storage

A solenoid stores energy in its magnetic field.

The stored energy is:

E = ½LI²

where:

  • E = energy in joules
  • L = inductance in henries
  • I = current in amperes

Increasing inductance allows more magnetic energy to be stored for the same current.


Worked Example: Energy Stored

A solenoid has:

L = 0.30 H

and carries:

I = 4.0 A

Use:

E = ½LI²

E = ½(0.30)(4.0²)

E = (0.15)(16)

E = 2.4 J

The energy is stored in the magnetic field of the solenoid.


What Happens When Current Increases?

When current begins increasing through a solenoid:

  • its magnetic field strengthens
  • magnetic flux increases
  • a self-induced EMF appears
  • the induced EMF opposes the increase

The larger the inductance, the greater this opposing EMF for a given rate of current change.

Therefore, a high-inductance solenoid tends to make rapid current changes more difficult.


What Happens When Current Decreases?

When current decreases:

  • magnetic field weakens
  • magnetic flux decreases
  • self-induced EMF is produced
  • the induced EMF acts to maintain the original current

The energy stored in the magnetic field can then be transferred back into the circuit.

This is why inductors can temporarily continue driving current when the original supply changes or is removed.


Inductors in Electrical Circuits

Real inductors are often constructed as coils or solenoids.

They are used because they can:

  • oppose rapid changes in current
  • store magnetic energy
  • filter electrical signals
  • smooth current variations
  • transfer and control energy in power circuits

Inductors appear in:

  • power supplies
  • filters
  • radios
  • amplifiers
  • motors
  • transformers
  • switching circuits
  • electronic converters
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7

Solenoids as Electromagnets and Inductors

The word solenoid is often used in two related ways.

In physics, a solenoid is a long coil of wire used to produce a magnetic field.

In practical devices, a solenoid may also contain a movable magnetic or iron component that converts electrical energy into mechanical motion.

Electrically, the coil still has inductance.

Therefore, when the current through a practical solenoid changes, self-induction occurs.


Practical Solenoid Devices

Solenoid coils are used in devices such as:

  • electromagnetic valves
  • relays
  • door locks
  • automotive systems
  • actuators
  • switching mechanisms

When these devices are switched on or off, their changing current produces self-induced EMF.

Circuit designers must account for this behaviour.


Ideal Solenoid vs Real Coil

The equation:

L = μN²A/l

is based on an ideal long solenoid.

Real coils may differ because:

  • magnetic fields are not perfectly uniform
  • some magnetic flux leaks outside the coil
  • the wire has resistance
  • core materials may behave nonlinearly
  • core permeability may change
  • coil geometry may not match the ideal model

Therefore, the equation provides an excellent model but may not exactly predict every real inductor.


Magnetic Saturation

In some magnetic-core inductors, increasing current eventually causes the core to approach magnetic saturation.

When this happens, the magnetic field no longer increases proportionally with current.

The effective inductance can decrease.

This means real magnetic-core inductors do not always have a perfectly constant inductance under all operating conditions.


Geometry Comparison Problem

Two solenoids use the same core material.

Solenoid B has:

  • twice the number of turns
  • twice the cross-sectional area
  • twice the length

Compare their inductances.

Use:

L ∝ N²A/l

Therefore:

L_B/L_A = (2²)(2)/2

L_B/L_A = 4

So:

Solenoid B has four times the inductance of Solenoid A.


Multiple-Change Example

A solenoid initially has inductance:

L₁ = 0.25 H

Its design is changed so that:

  • number of turns doubles
  • area triples
  • length doubles
  • core remains unchanged

Use:

L ∝ N²A/l

Therefore:

L₂/L₁ = (2²)(3)/(2)

L₂/L₁ = 6

Therefore:

L₂ = 6(0.25)

L₂ = 1.50 H


Radius and Length Example

A solenoid is redesigned so that:

  • its radius doubles
  • its length triples
  • number of turns remains constant
  • core material remains unchanged

Because:

A ∝ r²

doubling radius makes:

A → 4A

Length becomes:

l → 3l

Therefore:

L₂/L₁ = 4/3

So:

L₂ = 4L₁/3

The inductance increases by a factor of approximately:

1.33


A Complete Solenoid Problem

An air-core solenoid has:

N = 1500 turns

radius:

r = 1.5 cm

length:

l = 0.40 m

First convert radius:

r = 0.015 m

Calculate area:

A = πr²

A = π(0.015)²

A ≈ 7.07 × 10⁻⁴ m²

Now use:

L = μ₀N²A/l

L = (4π × 10⁻⁷)(1500²)(7.07 × 10⁻⁴)/(0.40)

Therefore:

L ≈ 5.0 × 10⁻³ H

or:

L ≈ 5.0 mH

This example shows why converting centimetres to metres before calculating area is essential.


A Reliable Strategy for Solenoid Problems

First identify:

  • N = number of turns
  • A = cross-sectional area
  • l = solenoid length
  • μ = permeability

Use:

L = μN²A/l

If radius is given, calculate:

A = πr²

before calculating inductance.

If self-induced EMF is required, use:

|ε| = L|ΔI/Δt|

If stored energy is required, use:

E = ½LI²

Always convert measurements into SI units before substituting.

Typical conversions include:

1 cm = 10⁻² m

1 cm² = 10⁻⁴ m²

1 mm = 10⁻³ m

1 mH = 10⁻³ H

1 μH = 10⁻⁶ H


Checking Your Answer

Ask:

  • Does increasing N increase L strongly?
  • Does increasing A increase L?
  • Does increasing l reduce L if N is fixed?
  • Does increasing μ increase L?
  • Did I square N?
  • Did I convert area correctly?
  • If radius changed, did I remember that A ∝ r²?
  • Are all quantities in SI units?
  • Does a larger L produce a larger induced EMF for the same ΔI/Δt?

These checks can catch many common errors.


Common Mistakes

Forgetting to square the number of turns

The equation is:

L = μN²A/l

not μNA/l.

Confusing inductance with induced EMF

Inductance is a property of the coil. Induced EMF occurs when the current changes.

Thinking inductance depends directly on current in the ideal model

For an ideal linear solenoid, L is determined by geometry and permeability, not by the instantaneous current.

Using diameter instead of radius in A = πr²

Always divide diameter by two first.

Failing to square the radius

Area depends on r².

Using centimetres directly in the equation

Convert lengths to metres and areas to square metres.

Thinking a longer coil always has greater inductance

For fixed N, A, and μ:

L ∝ 1/l

Ignoring what is held constant

If both N and l change, use the full relationship rather than considering only one variable.

Assuming real cores always have constant permeability

Real magnetic materials can show saturation and other nonlinear behaviour.


Key Terms

Inductance — property of a circuit describing its ability to produce self-induced EMF when current changes.

Henry (H) — SI unit of inductance.

Solenoid — long coil containing many closely spaced turns of wire.

Inductor — component designed to provide inductance in an electrical circuit.

Self-induction — production of an induced EMF by a circuit's own changing current.

Self-induced EMF — EMF generated by changing magnetic flux caused by changing current in the same circuit.

Magnetic flux — measure of magnetic field passing through a surface.

Flux linkage — magnetic flux linked with all turns of a coil.

Magnetic permeability — measure of how a material responds to and supports a magnetic field.

Relative permeability — permeability of a material compared with the permeability of free space.

Cross-sectional area — area enclosed by each turn perpendicular to the solenoid's axis.

Air-core solenoid — solenoid without a strongly magnetic core material.

Magnetic core — material placed inside a coil to modify and often strengthen its magnetic field.

Magnetic saturation — condition in which increasing magnetizing influence produces progressively less increase in a magnetic material's response.

Magnetic energy — energy stored in the magnetic field associated with current in an inductor.


Key Takeaways

  • Inductance measures how strongly a circuit produces self-induced EMF when its current changes.
  • Inductance is represented by L and measured in henries.
  • Solenoids behave as inductors because current produces magnetic flux through many turns.
  • Changing current produces changing magnetic flux and therefore self-induced EMF.
  • The induced EMF opposes the change in current according to Lenz's law.
  • For an ideal long solenoid, L = μN²A/l.
  • Inductance increases with magnetic permeability.
  • Inductance is proportional to the square of the number of turns.
  • Doubling the number of turns produces four times the inductance if other factors remain constant.
  • Inductance is directly proportional to cross-sectional area.
  • Because A = πr², increasing radius can strongly increase inductance.
  • For fixed N, A, and μ, increasing solenoid length decreases inductance.
  • Magnetic cores can greatly increase inductance by increasing magnetic flux.
  • Air-core and magnetic-core inductors are useful for different applications.
  • A larger inductance produces a larger self-induced EMF for the same rate of current change.
  • The magnitude of self-induced EMF is |ε| = L|ΔI/Δt|.
  • Inductors store energy in magnetic fields.
  • Stored energy is E = ½LI².
  • Coil geometry has a direct effect on electrical behaviour.
  • The ideal solenoid equation is a model; real coils can experience flux leakage, resistance, core losses, and magnetic saturation.

Check Your Understanding

  1. Define inductance and state its SI unit.
  2. Explain why a solenoid behaves as an inductor.
  3. Write the equation for the inductance of an ideal long solenoid and identify each quantity.
  4. A solenoid has its number of turns doubled while all other factors remain unchanged. By what factor does its inductance change?
  5. A solenoid has its number of turns tripled. What happens to its inductance if all other factors remain constant?
  6. Explain why increasing the cross-sectional area of a solenoid increases its inductance.
  7. A solenoid's radius is doubled while all other properties remain unchanged. By what factor does its inductance change?
  8. Explain what happens to inductance if the length of a solenoid is doubled while its number of turns, area, and core material remain constant.
  9. An air-core solenoid has 800 turns, area 3.0 × 10⁻⁴ m², and length 0.30 m. Using μ₀ = 4π × 10⁻⁷ H/m, calculate its inductance.
  10. A solenoid has L = 0.20 H and experiences a current change of 6.0 A in 0.30 s. Calculate the magnitude of its self-induced EMF.
  11. A 0.50 H solenoid carries a current of 3.0 A. Calculate the energy stored in its magnetic field.
  12. Two solenoids have identical area, length, and core material. One has 300 turns and the other has 900 turns. Compare their inductances.
  13. A solenoid is redesigned so that its number of turns doubles, its cross-sectional area doubles, and its length becomes four times greater. Determine the factor by which its inductance changes.
  14. Explain why inserting a suitable magnetic core into a solenoid can increase its inductance.
  15. An engineer wants to design a solenoid with a greater inductance without changing its core material. Describe at least three geometrical changes that could increase the inductance and explain each using L = μN²A/l.
 

2. Energy in Magnetic Fields

Learning outcomes
  • I can explain how inductors store energy.
  • I can describe magnetic field energy storage.
  • I can calculate energy stored in an inductor.
  • I can compare electrical and magnetic energy storage.
  • I can explain practical uses of stored magnetic energy.

Energy in Magnetic Fields

An inductor stores energy in the magnetic field produced by the current flowing through it.

When current through an inductor increases, the magnetic field becomes stronger. Because the changing magnetic field produces a self-induced EMF that opposes the increase in current, the power supply must do work to establish the current.

That work is stored as magnetic field energy.

When the current later decreases, the magnetic field collapses and the stored energy can be transferred back into the circuit.

The basic energy transfer is:

electrical energy → magnetic field energy → electrical energy


Energy Storage in an Inductor

Consider an inductor connected to a power supply.

When the circuit is first switched on:

  • current begins to increase
  • the magnetic field becomes stronger
  • magnetic flux through the coil increases
  • a self-induced EMF is produced
  • the self-induced EMF opposes the increase in current

The power supply must therefore transfer energy into the system.

Some of this energy becomes energy stored in the magnetic field surrounding and inside the inductor.


Why Energy Is Required

An inductor opposes a change in current because of Lenz's law.

As current increases, the self-induced EMF acts against that increase.

The source must therefore do work to move charge against the induced EMF.

The work done becomes stored magnetic energy.

This is similar to doing work to compress a spring. The work is not destroyed; it is stored and can later be released.


Energy Stored in an Inductor

The energy stored in an ideal inductor is:

E = ½LI²

where:

  • E = stored energy in joules (J)
  • L = inductance in henries (H)
  • I = current in amperes (A)

This is one of the most important equations for magnetic energy storage.


What the Equation Tells Us

From:

E = ½LI²

the stored energy depends on:

  • inductance
  • current

For a fixed current:

E ∝ L

For a fixed inductance:

E ∝ I²

Therefore, current has a particularly strong effect on the amount of stored energy.


Effect of Inductance

Suppose the current remains constant.

If inductance doubles:

L → 2L

then:

E → 2E

Therefore:

doubling inductance doubles the stored energy

for the same current.

A larger inductance means the circuit can store more magnetic energy at a given current.


Effect of Current

Stored energy is proportional to the square of current:

E ∝ I²

If current doubles:

I → 2I

then:

E → ½L(2I)²

E → 4(½LI²)

Therefore:

doubling current produces four times the stored energy

If current triples:

stored energy becomes nine times larger

assuming inductance remains constant.


Comparing Current and Inductance

Suppose an inductor initially stores energy E.

If its inductance doubles:

energy doubles

If its current doubles:

energy quadruples

This means that increasing current can have a much greater effect on stored energy than an equal proportional increase in inductance.


Worked Example: Stored Energy

An inductor has:

L = 0.50 H

and carries:

I = 4.0 A

Use:

E = ½LI²

E = ½(0.50)(4.0²)

E = (0.25)(16)

E = 4.0 J

The magnetic field stores:

4.0 J

of energy.


Worked Example: Smaller Inductor

An inductor has:

L = 25 mH

and carries:

I = 2.0 A

First convert:

25 mH = 0.025 H

Then:

E = ½LI²

E = ½(0.025)(2.0²)

E = (0.0125)(4.0)

E = 0.050 J


Worked Example: Finding Current

An inductor stores:

E = 9.0 J

and has:

L = 0.50 H

Start with:

E = ½LI²

Rearrange:

I² = 2E/L

I² = 2(9.0)/0.50

I² = 36

Therefore:

I = 6.0 A


Worked Example: Finding Inductance

An inductor stores:

E = 2.0 J

when carrying:

I = 4.0 A

Use:

E = ½LI²

Rearrange:

L = 2E/I²

L = 2(2.0)/(4.0²)

L = 4.0/16

L = 0.25 H


Why the Factor of One-Half Appears

The induced EMF is not constant while current increases from zero.

For an ideal linear inductor:

ε = L ΔI/Δt

As current builds, energy is progressively transferred into the magnetic field.

The total work required to increase current from zero to I gives:

E = ½LI²

The factor ½ appears because the energy is accumulated as the current and magnetic field build from zero to their final values.


Power During Energy Storage

Power is the rate of energy transfer:

P = VI

For an inductor:

V = L ΔI/Δt

Therefore:

P = LI ΔI/Δt

When current increases, energy is being transferred into the magnetic field.

When current decreases, stored magnetic energy can be transferred out of the inductor.


Energy Is Stored in the Field

It is common to say that energy is "stored in the inductor."

More precisely, the energy is associated with the magnetic field produced by the current.

For a solenoid, much of the magnetic field is concentrated:

  • inside the coil
  • and, if present, within its magnetic core

The stronger the field, the greater the magnetic energy that can be associated with the system.

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7

Magnetic Energy Density

Energy can also be described in terms of the amount stored per unit volume of magnetic field.

For a simple linear magnetic medium:

u = B²/(2μ)

where:

  • u = magnetic energy density in J/m³
  • B = magnetic field strength in T
  • μ = magnetic permeability

For free space:

u = B²/(2μ₀)

This equation shows that stronger magnetic fields contain greater energy density.


Energy in a Solenoid

For an ideal solenoid:

L = μN²A/l

and:

E = ½LI²

Combining these ideas shows that changing the geometry of a solenoid can affect its ability to store magnetic energy.

For the same current:

  • more turns generally increase stored energy
  • greater cross-sectional area increases stored energy
  • suitable magnetic cores can increase stored energy
  • changes in coil length affect inductance and therefore stored energy

Building the Magnetic Field

When an inductor is first connected to a DC supply, current does not immediately reach its final value.

Instead:

  1. current begins increasing
  2. magnetic field begins building
  3. self-induced EMF opposes the increase
  4. energy is transferred into the magnetic field
  5. current gradually approaches its steady value

Once the current becomes constant, the magnetic field becomes constant.

The stored energy remains:

E = ½LI²

as long as the current continues.


Releasing the Stored Energy

Suppose the current through an inductor begins to decrease.

The magnetic field begins collapsing.

According to Lenz's law, the inductor produces an EMF that attempts to maintain the current.

The magnetic field therefore transfers its stored energy back into the electrical circuit.

The sequence becomes:

magnetic field energy → electrical energy

This is why an inductor can continue driving current temporarily even after the original source is disconnected.

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9

Energy Conservation

Inductors provide a clear example of conservation of energy.

During current growth:

electrical energy supplied → magnetic field energy

During current decay:

magnetic field energy → electrical energy

In a real circuit, some energy also becomes thermal energy because wires and other components have resistance.

Therefore, a real energy pathway might be:

electrical energy → magnetic field energy → electrical energy + thermal energy


Ideal and Real Inductors

An ideal inductor has no electrical resistance and no energy losses.

It can theoretically store and return magnetic energy without loss.

A real inductor has:

  • wire resistance
  • magnetic-core losses
  • eddy-current losses
  • hysteresis losses
  • magnetic flux leakage

Therefore, some energy is converted into unwanted thermal energy.


Resistance vs Inductance

Resistance and inductance affect electrical energy differently.

A resistor mainly converts electrical energy into thermal energy:

electrical energy → thermal energy

An ideal inductor temporarily stores energy:

electrical energy → magnetic field energy → electrical energy

This distinction is important.

An inductor does not simply "use up" energy in the same way as a resistor.


Electrical Energy Storage

Electrical systems can store energy in different forms.

Two important components are:

  • capacitors
  • inductors

A capacitor stores energy in an electric field.

An inductor stores energy in a magnetic field.

These two devices play complementary roles in many electrical circuits.


Capacitors and Inductors

Capacitor Inductor
Stores energy in an electric field Stores energy in a magnetic field
Energy depends on voltage Energy depends on current
E = ½CV² E = ½LI²
Opposes rapid changes in voltage Opposes rapid changes in current
Uses capacitance C Uses inductance L
Capacitance measured in farads Inductance measured in henries

This comparison is extremely useful when studying electrical energy storage.


Similarity Between the Energy Equations

For a capacitor:

E_C = ½CV²

For an inductor:

E_L = ½LI²

Notice the similar structure.

For capacitors:

  • C describes the component
  • V describes its electrical state

For inductors:

  • L describes the component
  • I describes its electrical state

In both cases, stored energy depends on the square of the electrical quantity.


Comparing Energy Storage

Consider:

Capacitor: E = ½CV²

Inductor: E = ½LI²

If voltage across a capacitor doubles:

capacitor energy becomes 4 times larger

If current through an inductor doubles:

inductor energy becomes 4 times larger

Both systems therefore show a squared dependence.


Batteries Are Different

A battery also stores energy, but primarily as chemical energy, not as electric or magnetic field energy.

Therefore:

battery → chemical energy

capacitor → electric field energy

inductor → magnetic field energy

These devices can all supply electrical energy to circuits, but they store energy in fundamentally different ways.


Inductor and Capacitor Energy Exchange

A capacitor and inductor can exchange energy with each other.

Suppose a charged capacitor is connected to an inductor.

Initially, much of the energy may be stored in the capacitor's electric field.

As the capacitor discharges:

  • current increases
  • the inductor's magnetic field strengthens
  • energy moves into the magnetic field

Later, the magnetic field collapses and can recharge the capacitor.

In an ideal system:

electric field energy ↔ magnetic field energy

This behaviour is the basis of LC oscillations.

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7

Energy in an LC Circuit

At one moment, the capacitor may have maximum voltage and the current may be zero.

Energy is mainly:

electric field energy

Later, the capacitor voltage decreases while current increases.

Energy moves into the inductor.

When current reaches its maximum, energy is mainly:

magnetic field energy

The process can then reverse.

Real circuits gradually lose energy because of resistance.


Practical Use: Switching Power Supplies

Modern electronic power supplies frequently use inductors to temporarily store energy.

A switching circuit rapidly changes the current through an inductor.

During part of the switching cycle:

energy is stored in the magnetic field

During another part:

energy is released to the circuit

This allows efficient conversion between different voltage and current levels.

Inductors are therefore important in devices such as:

  • phone chargers
  • computer power supplies
  • LED drivers
  • battery-powered electronics

Buck Converters

A buck converter reduces DC voltage.

An inductor helps maintain relatively smooth current while electronic switches repeatedly turn on and off.

During part of the cycle, the inductor stores magnetic energy.

During another part, it releases energy to the load.

This helps convert electrical power efficiently.


Boost Converters

A boost converter can produce an output voltage greater than its input voltage.

Current first builds through an inductor.

The inductor stores energy in its magnetic field.

When the switching configuration changes, the collapsing magnetic field produces an induced voltage.

The stored energy is transferred to the output.

This demonstrates a direct practical use of:

E = ½LI²


Practical Use: Electrical Filters

Inductors are also used to smooth current.

Because an inductor opposes rapid current changes, it can reduce unwanted fluctuations.

Energy is alternately stored and released as the current changes.

This is useful in:

  • power supplies
  • audio circuits
  • communication systems
  • electronic filters

Practical Use: Ignition Systems

Inductive energy storage can be used to produce large voltages.

Current is first established through a coil.

Energy is stored in its magnetic field.

When the current is interrupted rapidly:

  • magnetic field collapses
  • flux changes rapidly
  • a large induced EMF can be produced

This principle is used in some ignition and pulsed electrical systems.


Practical Use: Electromagnets

An electromagnet stores energy in its magnetic field while current flows.

Examples include:

  • relays
  • solenoids
  • electromagnetic actuators
  • lifting magnets
  • magnetic valves

When the current is switched off, the stored magnetic energy must go somewhere.

Circuit designers therefore need to manage the released energy safely.


Voltage Spikes

The energy stored in an inductor cannot disappear instantly.

If a current-carrying inductor is suddenly disconnected, the current attempts to decrease very rapidly.

Since:

|ε| = L|ΔI/Δt|

a very rapid change can produce a large voltage.

This voltage may cause:

  • sparks
  • damage to electronic components
  • electrical interference

Protective circuits are often used to provide a safe path for the stored energy.


Flyback Protection

A coil controlled electronically may have a protective path added across it.

When the switch opens:

  • the magnetic field collapses
  • the inductor attempts to maintain current
  • stored energy continues circulating through the protective path
  • the current gradually decreases
  • the energy is safely dissipated

This helps protect sensitive switching components from large induced voltages.

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7

Energy Storage in Electric Vehicles

Inductors are important components in the power electronics used in electric vehicles.

They help:

  • convert voltages
  • control motor currents
  • smooth electrical power
  • temporarily store magnetic energy
  • manage energy transfer between batteries, motors, and electronic systems

The energy stored in an individual inductor may be temporary, but repeated storage and release can occur thousands of times per second.


Renewable Energy Systems

Power converters used with:

  • solar panels
  • wind turbines
  • battery storage

often contain inductors.

The inductors temporarily store and release magnetic energy as electronic switches control the flow of electrical power.

This helps convert variable electrical inputs into forms suitable for:

  • batteries
  • electrical grids
  • motors
  • electronic equipment

Magnetic Energy and Current Changes

The relationship between energy and current helps explain why inductors resist changes in current.

If current increases:

magnetic energy must increase

That requires an energy input.

If current decreases:

magnetic energy decreases

That energy must be transferred elsewhere.

Therefore, changing current involves changing the amount of energy stored in the magnetic field.


Worked Comparison

Inductor A:

L = 0.20 H

I = 4.0 A

Energy:

E_A = ½(0.20)(4.0²)

E_A = 1.6 J

Inductor B:

L = 0.40 H

I = 4.0 A

Energy:

E_B = ½(0.40)(4.0²)

E_B = 3.2 J

Doubling inductance has doubled the stored energy.


Current Comparison

An inductor has:

L = 0.50 H

At:

I₁ = 2.0 A

E₁ = ½(0.50)(2.0²)

E₁ = 1.0 J

At:

I₂ = 4.0 A

E₂ = ½(0.50)(4.0²)

E₂ = 4.0 J

The current doubled, but the stored energy increased by a factor of four.


Multiple-Change Example

Suppose an inductor initially has:

L₁ = L

I₁ = I

Its inductance doubles and its current triples.

Since:

E = ½LI²

the new energy factor is:

2 × 3²

= 2 × 9

= 18

Therefore:

the new magnetic energy is 18 times the original energy.


A Complete Calculation

An inductor has:

L = 0.80 H

The current increases from zero to:

I = 5.0 A

Calculate the final stored energy.

E = ½LI²

E = ½(0.80)(5.0²)

E = (0.40)(25)

E = 10 J

If the current later decreases to:

I = 3.0 A

the remaining energy is:

E = ½(0.80)(3.0²)

E = (0.40)(9)

E = 3.6 J

Energy released:

10 − 3.6

6.4 J

Therefore, 6.4 J of magnetic energy has been transferred out of the inductor.


Comparing an Inductor and Capacitor

An inductor has:

L = 2.0 H

I = 3.0 A

Its energy is:

E_L = ½(2.0)(3.0²)

E_L = 9.0 J

A capacitor has:

C = 0.020 F

V = 30 V

Its energy is:

E_C = ½(0.020)(30²)

E_C = (0.010)(900)

E_C = 9.0 J

Both devices store the same amount of energy, but:

  • the inductor stores it in a magnetic field
  • the capacitor stores it in an electric field

A Reliable Strategy for Energy Problems

First identify:

  • inductance L
  • current I

Convert units if necessary.

Then use:

E = ½LI²

If current is unknown:

I = √(2E/L)

If inductance is unknown:

L = 2E/I²

For comparisons, remember:

E ∝ L

and:

E ∝ I²

If the problem asks how much energy is released as current changes:

energy released = E_initial − E_final


Unit Conversions

Inductance must usually be converted into henries.

Remember:

1 mH = 10⁻³ H

1 μH = 10⁻⁶ H

For example:

50 mH = 0.050 H

250 mH = 0.250 H

20 μH = 2.0 × 10⁻⁵ H

Current should normally be expressed in amperes.

Energy is then obtained in joules.


Common Mistakes

Forgetting to square the current

The equation is:

E = ½LI²

not ½LI.

Forgetting the factor ½

The factor one-half is essential.

Using millihenries as though they were henries

Always convert units before calculating.

Thinking the energy is stored in the electric current itself

The energy is associated with the magnetic field produced by the current.

Thinking an ideal inductor permanently consumes energy

An ideal inductor can store energy and later return it.

Confusing an inductor with a resistor

A resistor dissipates energy mainly as heat; an ideal inductor stores magnetic energy.

Confusing magnetic and electric energy storage

Inductors store magnetic field energy. Capacitors store electric field energy.

Assuming the energy disappears when current falls

The stored energy must be transferred somewhere else.

Ignoring voltage spikes when interrupting current

A rapid decrease in current can produce a large induced EMF.


Key Terms

Magnetic field energy — energy associated with a magnetic field.

Inductor — circuit component that stores energy in a magnetic field and opposes changes in current.

Inductance — measure of a circuit's self-inductive behaviour, represented by L.

Henry (H) — SI unit of inductance.

Self-induction — production of an EMF caused by changes in a circuit's own current.

Self-induced EMF — voltage produced by changing magnetic flux caused by changing current in the same circuit.

Lenz's law — principle stating that induced effects oppose the change that produced them.

Energy density — energy stored per unit volume.

Capacitor — component that stores energy in an electric field.

Electric field energy — energy associated with an electric field, such as that between capacitor plates.

Magnetic flux — measure of magnetic field passing through a surface.

RL circuit — circuit containing resistance and inductance.

LC circuit — circuit containing inductance and capacitance that can exchange energy between magnetic and electric fields.

Flyback protection — circuit arrangement used to safely manage energy released when current through an inductive load is interrupted.

Energy conservation — principle that energy cannot be created or destroyed, only transferred or transformed.


Key Takeaways

  • Inductors store energy in magnetic fields.
  • Energy must be supplied to establish the magnetic field around an inductor.
  • Self-induction opposes the increase in current while the magnetic field is being established.
  • The energy stored in an inductor is E = ½LI².
  • Stored energy is directly proportional to inductance.
  • Stored energy is proportional to the square of current.
  • Doubling inductance doubles the stored energy for the same current.
  • Doubling current quadruples the stored energy.
  • When current decreases, the magnetic field collapses and stored energy is released.
  • Magnetic energy can be transferred back into the electrical circuit.
  • Energy conservation applies throughout the storage and release process.
  • Real inductors lose some energy through resistance and magnetic-core effects.
  • Capacitors store energy in electric fields, while inductors store energy in magnetic fields.
  • Capacitor energy is E = ½CV².
  • Inductor energy is E = ½LI².
  • Inductors oppose rapid changes in current, while capacitors oppose rapid changes in voltage.
  • LC circuits can exchange energy between electric and magnetic fields.
  • Sudden interruption of current can release stored magnetic energy as a large induced voltage.
  • Inductors are important in power converters, filters, motor controllers, renewable-energy systems, and many other electronic devices.
  • Magnetic energy storage allows circuits to control and transfer electrical energy efficiently.
 
 
 

3. RL Circuits

Learning outcomes
  • I can describe the behavior of resistor-inductor (RL) circuits.
  • I can explain why current changes gradually in RL circuits.
  • I can interpret current-time graphs for RL circuits.
  • I can explain the concept of the RL time constant.
  • I can solve simple RL circuit problems.

RL Circuits

An RL circuit is a circuit containing both a resistor (R) and an inductor (L). One of the most important features of an RL circuit is that its current cannot change instantly.

When a voltage is applied, the current rises gradually. When the voltage source is removed, the current falls gradually.

This happens because the changing current produces a changing magnetic field in the inductor. The changing magnetic flux creates a self-induced EMF that opposes the change in current.

The basic idea is:

changing current → changing magnetic field → self-induced EMF → opposition to the change in current

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8

The Components of an RL Circuit

A simple series RL circuit contains:

  • a voltage source
  • a resistor
  • an inductor
  • connecting wires
  • often a switch

The same current flows through the resistor and inductor because they are connected in series.

The resistor obeys:

V_R = IR

The inductor produces an induced voltage when current changes:

V_L = L ΔI/Δt

The inductor's induced effect opposes the change in current.


What Happens When the Switch Is Closed?

Imagine an RL circuit connected to a DC battery.

Before the switch closes:

I = 0

When the switch closes, the battery attempts to establish a current.

However, as the current begins increasing:

  • the inductor's magnetic field begins increasing
  • magnetic flux changes
  • self-induced EMF is produced
  • the induced EMF opposes the increase in current

Therefore, the current does not immediately reach its final value.

Instead:

current rises gradually


Why Current Cannot Change Instantly

The induced EMF of an inductor is related to the rate of current change:

|ε| = L|ΔI/Δt|

Imagine the current changed instantly.

Then:

Δt → 0

which would make:

ΔI/Δt

extremely large.

The corresponding induced voltage would also become extremely large.

Therefore, an ideal inductor prevents instantaneous changes in current.

An important circuit rule is:

current through an ideal inductor must change continuously.


Current Growth

When a DC voltage is first applied to a series RL circuit, current begins at zero and gradually approaches a maximum value.

The current is described by:

I = I_max(1 − e^(−t/τ))

where:

  • I = current at time t
  • I_max = final steady current
  • t = time
  • τ = RL time constant
  • e ≈ 2.718

The curve rises rapidly at first and then gradually levels off.

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7

Interpreting the Current-Growth Graph

At:

t = 0

the current is:

I = 0

Initially, the current increases rapidly.

As time passes, the rate of increase becomes smaller.

Eventually:

I → I_max

The curve approaches the final value asymptotically.

In practical calculations, the current is considered very close to its final value after several time constants.


Final Current

Once the current becomes steady:

ΔI/Δt = 0

Therefore, the self-induced EMF becomes zero.

For an ideal inductor in a DC circuit, the final current is determined by the resistance:

I_max = V/R

where:

  • V = supply voltage
  • R = total circuit resistance

The inductor strongly affects how quickly the current reaches this value, but an ideal inductor does not change the final steady-state current.


Example: Final Current

An RL circuit contains:

V = 12 V

R = 6.0 Ω

L = 2.0 H

Once the current becomes steady:

I_max = V/R

I_max = 12/6.0

I_max = 2.0 A

The inductance affects how quickly the current approaches 2.0 A.


The RL Time Constant

The rate at which current changes is described using the time constant.

For an RL circuit:

τ = L/R

where:

  • τ = time constant in seconds (s)
  • L = inductance in henries (H)
  • R = resistance in ohms (Ω)

The time constant tells us approximately how quickly the circuit responds to a change.


Meaning of the Time Constant

During current growth, after one time constant:

t = τ

the current has reached approximately:

63% of its final value

Therefore:

I ≈ 0.63I_max

After two time constants:

I ≈ 0.86I_max

After three:

I ≈ 0.95I_max

After four:

I ≈ 0.98I_max

After five:

I ≈ 0.99I_max

After about 5τ, the current is normally treated as essentially steady.


Current Growth Table

Time Approximate Current
0 0% of I_max
1τ 63% of I_max
2τ 86% of I_max
3τ 95% of I_max
4τ 98% of I_max
5τ 99% of I_max

This pattern is useful for interpreting RL current-time graphs without performing detailed exponential calculations.


Worked Example: Finding the Time Constant

An RL circuit contains:

L = 3.0 H

R = 6.0 Ω

Use:

τ = L/R

τ = 3.0/6.0

τ = 0.50 s

After:

0.50 s

the current has reached approximately 63% of its final value.

After approximately:

5τ = 5(0.50)

5τ = 2.5 s

the current is essentially at its steady value.


Worked Example: Current After One Time Constant

An RL circuit has a final current:

I_max = 8.0 A

After one time constant:

I ≈ 0.63I_max

I ≈ (0.63)(8.0)

I ≈ 5.0 A


Effect of Inductance on the Time Constant

From:

τ = L/R

increasing inductance increases the time constant.

Therefore:

larger L → larger τ → slower current change

A larger inductor produces a greater self-induced EMF for the same rate of current change.

It therefore takes longer for the current to reach its steady value.


Effect of Resistance on the Time Constant

From:

τ = L/R

increasing resistance decreases the time constant.

Therefore:

larger R → smaller τ

However, increasing resistance also reduces the final current because:

I_max = V/R

So resistance affects both:

  • the final current
  • the time constant

These effects should not be confused.


Comparing Two RL Circuits

Circuit A:

L = 2.0 H

R = 4.0 Ω

Therefore:

τ_A = 2.0/4.0

τ_A = 0.50 s

Circuit B:

L = 4.0 H

R = 4.0 Ω

Therefore:

τ_B = 4.0/4.0

τ_B = 1.0 s

Circuit B has the greater inductance and therefore responds more slowly.


Current at Any Time During Growth

The full current-growth equation is:

I = I_max(1 − e^(−t/τ))

This allows the current to be calculated at any time.

Remember:

I_max = V/R

and:

τ = L/R


Worked Example: Current During Growth

An RL circuit has:

V = 12 V

R = 4.0 Ω

L = 2.0 H

Find the current after:

t = 0.50 s

First calculate the final current:

I_max = V/R

I_max = 12/4.0

I_max = 3.0 A

Now calculate the time constant:

τ = L/R

τ = 2.0/4.0

τ = 0.50 s

Therefore:

t = τ

After one time constant, the current is approximately 63% of its final value:

I ≈ 0.63(3.0)

I ≈ 1.9 A


Using the Exponential Equation

For the same circuit:

I = I_max(1 − e^(−t/τ))

I = 3.0(1 − e^(−0.50/0.50))

I = 3.0(1 − e⁻¹)

Since:

e⁻¹ ≈ 0.368

I = 3.0(1 − 0.368)

I = 3.0(0.632)

I ≈ 1.90 A

This agrees with the 63% time-constant rule.


What Happens to the Inductor Voltage?

When the circuit is first switched on, the current is changing most rapidly.

Therefore, the inductor's induced voltage is largest.

As the current approaches its steady value:

  • current changes more slowly
  • induced voltage decreases

Eventually:

ΔI/Δt = 0

and:

V_L = 0

for an ideal inductor under steady DC conditions.


Voltage Across the Resistor

The resistor voltage is:

V_R = IR

Immediately after switching on:

I = 0

so:

V_R = 0

As current increases:

V_R increases

Eventually:

I = V/R

so:

V_R = V

for the ideal series RL circuit.


Voltage Changes During Current Growth

The behaviour can be summarized:

Time Current Resistor Voltage Inductor Voltage
Immediately after switch closes 0 0 Maximum
During growth Increasing Increasing Decreasing
Long after switch closes Maximum and steady Supply voltage 0

This demonstrates how the inductor initially opposes the establishment of current.


Kirchhoff's Voltage Law in an RL Circuit

At any moment during current growth:

V = V_R + V_L

Therefore:

V = IR + L ΔI/Δt

The supply voltage is shared between the resistor and the inductor.

Initially, most of the voltage appears across the inductor.

Later, as current becomes steady, most or all of the supply voltage appears across the resistor in the ideal model.


Energy During Current Growth

While current increases, the inductor stores energy in its magnetic field.

The stored energy is:

E = ½LI²

As current increases:

  • magnetic field strengthens
  • stored magnetic energy increases

At the final steady current:

E_max = ½LI_max²


Worked Example: Final Stored Energy

An RL circuit contains:

L = 2.0 H

V = 12 V

R = 6.0 Ω

Final current:

I_max = V/R

I_max = 12/6.0

I_max = 2.0 A

Stored energy:

E = ½LI²

E = ½(2.0)(2.0²)

E = 4.0 J


Switching the Circuit Off

Suppose an inductor is carrying a steady current and the supply is removed while a closed path remains available for the current.

The current attempts to decrease.

The magnetic field begins collapsing.

This produces a self-induced EMF that acts to maintain the original current.

Therefore:

the current decreases gradually rather than instantly

This process is called current decay.

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7

Current Decay

For a simple RL decay circuit:

I = I₀e^(−t/τ)

where:

  • I = current at time t
  • I₀ = initial current
  • τ = L/R
  • t = time

The current decreases exponentially.

It approaches zero but does not mathematically reach exactly zero in the ideal exponential model.


Interpreting the Current-Decay Graph

At:

t = 0

the current is:

I = I₀

After one time constant:

I ≈ 0.37I₀

After two:

I ≈ 0.14I₀

After three:

I ≈ 0.050I₀

After four:

I ≈ 0.018I₀

After five:

I ≈ 0.007I₀

So after approximately five time constants, the current is usually treated as essentially zero.


Current Decay Table

Time Current Remaining
0 100%
1τ 37%
2τ 14%
3τ 5%
4τ 2%
5τ Less than 1%

Notice the connection:

During growth after one τ:

63% reached

During decay after one τ:

37% remains

because:

63% + 37% = 100%

approximately.


Worked Example: Current Decay

An inductor initially carries:

I₀ = 6.0 A

The circuit has:

L = 2.0 H

R = 4.0 Ω

Calculate the time constant:

τ = L/R

τ = 2.0/4.0

τ = 0.50 s

After one time constant:

I ≈ 0.37I₀

I ≈ 0.37(6.0)

I ≈ 2.2 A


Current After Two Time Constants

Using the same circuit:

t = 2τ

Approximately 14% of the original current remains.

I ≈ 0.14(6.0)

I ≈ 0.84 A

Using the exponential equation gives approximately the same result.


Growth vs Decay Graphs

The two graphs have different shapes.

Current growth:

  • begins at zero
  • rises rapidly at first
  • gradually levels off
  • approaches I_max

Current decay:

  • begins at I₀
  • falls rapidly at first
  • gradually levels off
  • approaches zero

Both are exponential curves.


Reading the Time Constant from a Graph

For a current-growth graph:

  1. identify the final current I_max
  2. calculate 63% of I_max
  3. find where the curve reaches this value
  4. read the corresponding time

That time is approximately:

τ

For a current-decay graph:

  1. identify the initial current I₀
  2. calculate 37% of I₀
  3. find where the curve reaches this value
  4. read the corresponding time

That time is approximately:

τ


Example: Finding τ from a Growth Graph

Suppose a graph approaches a final current of:

10 A

Calculate 63%:

0.63(10)

6.3 A

If the graph reaches 6.3 A at:

0.40 s

then:

τ = 0.40 s

If R = 5.0 Ω, then:

τ = L/R

so:

L = τR

L = (0.40)(5.0)

L = 2.0 H


Example: Finding τ from a Decay Graph

Suppose current begins at:

8.0 A

After one time constant, the current should be:

0.37(8.0)

≈ 3.0 A

If the graph reaches approximately 3.0 A at:

0.25 s

then:

τ ≈ 0.25 s


Comparing Different Time Constants

A circuit with a small time constant changes current quickly.

Its current-time graph is relatively steep.

A circuit with a large time constant changes current more slowly.

Its graph is more gradual.

Therefore:

larger τ → slower response

smaller τ → faster response


Effect of Increasing Inductance on the Graph

If resistance remains constant and inductance increases:

τ = L/R

so τ increases.

The current-growth graph becomes more gradual.

The circuit takes longer to approach its final current.

Similarly, during decay, the current remains significant for a longer time.


Effect of Increasing Resistance on the Graph

If inductance remains constant and resistance increases:

τ = L/R

so τ decreases.

The current responds more quickly.

However, during current growth from a fixed-voltage supply:

I_max = V/R

also decreases.

Therefore, increasing resistance changes both:

  • the time scale
  • the final current

This is an important point when comparing graphs.


Complete Growth Problem

A series RL circuit contains:

V = 24 V

R = 8.0 Ω

L = 4.0 H

Find the final current, time constant, and current after one time constant.

Final current:

I_max = V/R

I_max = 24/8.0

I_max = 3.0 A

Time constant:

τ = L/R

τ = 4.0/8.0

τ = 0.50 s

After one time constant:

I ≈ 0.63I_max

I ≈ 0.63(3.0)

I ≈ 1.9 A

After about:

5τ = 2.5 s

the current is essentially at its final value.


Complete Decay Problem

An RL circuit initially carries:

I₀ = 5.0 A

The circuit has:

L = 1.5 H

R = 3.0 Ω

Time constant:

τ = L/R

τ = 1.5/3.0

τ = 0.50 s

Find the current after:

t = 1.0 s

Since:

1.0 s = 2τ

approximately 14% remains:

I ≈ 0.14(5.0)

I ≈ 0.70 A

Using the exact equation:

I = I₀e^(−t/τ)

I = 5.0e^(−1.0/0.50)

I = 5.0e⁻²

I ≈ 5.0(0.135)

I ≈ 0.68 A


Finding Time Using the Exponential Equation

Sometimes the unknown is time.

For decay:

I = I₀e^(−t/τ)

Suppose the current falls to half its initial value:

I/I₀ = 0.50

Then:

0.50 = e^(−t/τ)

Taking the natural logarithm:

ln(0.50) = −t/τ

Therefore:

t = −τ ln(0.50)

Since:

ln(0.50) ≈ −0.693

then:

t ≈ 0.693τ

So an RL decay does not take one full time constant to fall to half its initial current.


Energy During Current Decay

As current decreases, the magnetic energy:

E = ½LI²

also decreases.

The collapsing magnetic field transfers energy back into the circuit.

In a simple resistor-inductor decay circuit, much of this energy eventually becomes thermal energy in the resistor.

Therefore:

magnetic field energy → electrical energy → thermal energy


Why Switching an Inductor Can Produce a Large Voltage

If the circuit is opened suddenly without a suitable current path, the current attempts to fall very rapidly.

From:

|ε| = L|ΔI/Δt|

a very large rate of change of current can produce a very large induced voltage.

This can cause:

  • sparks across switches
  • damage to electronic components
  • electrical interference

Practical circuits often provide a safe path for the current to decay.


Flyback Protection

Coils in relays, motors, and solenoids can behave as inductive loads.

When they are switched off, their stored magnetic energy must be released.

A protective component such as a flyback diode can provide a temporary current path.

The current then decreases gradually instead of producing a damaging voltage spike.

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8

Practical Uses of RL Behavior

RL circuits appear wherever coils and changing currents are present.

Examples include:

  • electromagnets
  • relays
  • solenoids
  • electric motors
  • transformers
  • power supplies
  • electronic filters
  • switching circuits

In each case, inductance affects how rapidly current can change.


RL Circuits in Electromagnets

An electromagnet contains a coil with inductance.

When switched on:

  • current gradually increases
  • magnetic field gradually strengthens

When switched off:

  • current gradually decreases if a path remains
  • magnetic field collapses
  • stored energy is released

The time constant therefore influences how quickly the electromagnet responds.


RL Circuits in Motors

Motor windings have both:

  • resistance
  • inductance

They therefore behave partly like RL circuits.

The inductance prevents motor current from changing instantly.

This affects:

  • starting behaviour
  • current control
  • switching
  • motor speed control
  • electronic drive design

RL Circuits and Filters

Inductors oppose rapid current changes.

This makes them useful in electrical filters.

Rapidly changing signals can experience stronger inductive effects than slowly changing signals.

RL networks can therefore help:

  • reduce electrical noise
  • separate signals by frequency
  • smooth current
  • shape electrical signals

RL Circuits vs Purely Resistive Circuits

A purely resistive DC circuit responds almost immediately in the ideal model.

Its current is:

I = V/R

An RL circuit behaves differently during switching because the inductor produces self-induced EMF.

Pure Resistor Circuit RL Circuit
No significant inductance Contains inductance
Current changes essentially immediately in ideal model Current changes gradually
No magnetic energy storage Stores magnetic energy
I determined by V/R Final I determined by V/R
No RL time constant τ = L/R

RL Circuits and RC Circuits

RL and RC circuits both show exponential behaviour, but they involve different quantities.

RL Circuit RC Circuit
Resistor + inductor Resistor + capacitor
Current changes gradually Capacitor voltage changes gradually
Stores magnetic energy Stores electric-field energy
τ = L/R τ = RC
Inductor opposes current change Capacitor opposes voltage change

Both systems are important examples of circuits with time-dependent behaviour.


A Reliable Strategy for RL Problems

First identify:

  • V = supply voltage
  • R = resistance
  • L = inductance
  • t = time

Calculate the time constant:

τ = L/R

For current growth, calculate the final current:

I_max = V/R

Then use either the approximate time-constant percentages or:

I = I_max(1 − e^(−t/τ))

For current decay use:

I = I₀e^(−t/τ)

Remember:

growth at 1τ → 63%

decay at 1τ → 37% remaining

After approximately:

5τ

the change is essentially complete.


Common Mistakes

Thinking current changes instantly in an RL circuit

Inductance opposes changes in current.

Thinking the inductor stops current permanently

The inductor mainly affects changing current. With steady DC, an ideal inductor has zero induced voltage.

Using τ = R/L

For an RL circuit:

τ = L/R

Confusing 63% and 37%

During growth after one τ:

63% of final current has been reached.

During decay after one τ:

37% of initial current remains.

Thinking the time constant is the time required to complete the change

The exponential process is not mathematically complete after one τ. One τ describes a characteristic fraction of the change.

Forgetting to calculate the final current

For a simple DC series RL circuit:

I_max = V/R

Using the growth equation for decay

Growth:

I = I_max(1 − e^(−t/τ))

Decay:

I = I₀e^(−t/τ)

Thinking resistance only affects the time constant

Resistance also affects the final current.

Ignoring stored magnetic energy

During current decay, the magnetic field releases energy back into the circuit.


Key Terms

RL circuit — circuit containing resistance and inductance.

Resistor — component that opposes current and dissipates electrical energy, commonly as thermal energy.

Inductor — component that stores energy in a magnetic field and opposes changes in current.

Inductance — measure of an inductor's ability to produce self-induced EMF.

Self-induction — production of an EMF caused by a circuit's own changing current.

Self-induced EMF — induced voltage produced when a circuit's own magnetic flux changes.

Steady state — condition in which current has stopped changing with time.

Transient — temporary period during which current or voltage changes from one steady condition toward another.

Time constant — characteristic time describing how quickly an RL circuit responds.

Current growth — exponential increase of current toward its final value after a DC source is applied.

Current decay — exponential decrease of current after the source is removed while a suitable current path remains.

Exponential change — change whose rate depends on how far the system remains from its final state.

Magnetic energy — energy stored in the magnetic field of an inductor.

Flyback diode — protective component providing a current path for an inductive load when it is switched off.


Key Takeaways

  • An RL circuit contains both resistance and inductance.
  • Current cannot change instantly through an ideal inductor.
  • Self-induction causes the inductor to oppose changes in current.
  • When a DC source is connected, current rises gradually toward its final value.
  • The final current in a simple ideal series RL circuit is I_max = V/R.
  • The RL time constant is τ = L/R.
  • Larger inductance produces a larger time constant and slower current response.
  • Larger resistance produces a smaller time constant when inductance remains fixed.
  • After one time constant during growth, current reaches about 63% of its final value.
  • After one time constant during decay, about 37% of the original current remains.
  • After approximately five time constants, the transition is normally considered essentially complete.
  • Current growth follows I = I_max(1 − e^(−t/τ)).
  • Current decay follows I = I₀e^(−t/τ).
  • Current-time graphs for RL circuits are exponential rather than straight lines.
  • During switch-on, inductor voltage is initially large and decreases toward zero.
  • During switch-on, resistor voltage increases as current increases.
  • Inductors store energy according to E = ½LI².
  • During current decay, stored magnetic energy is transferred back into the circuit.
  • Rapidly interrupting an inductive current can produce a large voltage.
  • RL behaviour is important in motors, relays, electromagnets, power supplies, filters, and switching circuits.

Check Your Understanding

  1. What is an RL circuit?
  2. Explain why current cannot change instantly through an ideal inductor.
  3. Describe what happens to the current immediately after a DC source is connected to an RL circuit.
  4. A circuit contains L = 4.0 H and R = 8.0 Ω. Calculate its time constant.
  5. Explain what a time constant of 0.50 s means during current growth.
  6. An RL circuit has a final current of 10 A. Approximately what current flows after one time constant?
  7. A current begins at 8.0 A and decays through an RL circuit. Approximately what current remains after one time constant?
  8. A 12 V supply is connected to a series RL circuit containing R = 3.0 Ω and L = 1.5 H. Calculate the final current and time constant.
  9. For the circuit in Question 8, estimate the current after one time constant.
  10. An RL circuit has I_max = 6.0 A and τ = 0.40 s. Calculate the current after 0.80 s using I = I_max(1 − e^(−t/τ)).
  11. An inductor initially carries 5.0 A in a circuit with τ = 0.25 s. Calculate the current remaining after 0.50 s.
  12. Describe the shape of a current-time graph when an RL circuit is switched on. How would increasing inductance change the graph?
  13. Explain how the voltage across the resistor and the voltage across the inductor change from the moment a DC RL circuit is switched on until steady state is reached.
  14. Explain where the energy stored in an inductor goes when the current through an RL circuit decreases.
  15. Two RL circuits have the same resistance, but Circuit A has twice the inductance of Circuit B. Compare their time constants and explain which circuit's current changes more slowly.

4. Mutual Inductance

Learning outcomes
  • I can define mutual inductance.
  • I can explain how energy is transferred between coils.
  • I can identify factors affecting mutual inductance.
  • I can compare mutual inductance with self-inductance.
  • I can explain how mutual inductance is used in electrical devices.

Mutual Inductance

Mutual inductance describes the ability of a changing current in one circuit to produce an induced EMF in another nearby circuit.

When current in the first coil changes, its magnetic field changes. If some of this changing magnetic field passes through a second coil, the magnetic flux through the second coil changes. According to Faraday's law, this changing flux produces an induced EMF.

The process can be summarized as:

changing current in Coil 1 → changing magnetic field → changing flux through Coil 2 → induced EMF in Coil 2

Mutual inductance allows electrical energy and signals to be transferred between circuits without requiring a direct electrical connection.

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8

Defining Mutual Inductance

The strength of the electromagnetic interaction between two circuits is measured by their mutual inductance.

The symbol is:

M

The SI unit is the:

henry (H)

For two coils, the magnitude of the induced EMF in Coil 2 can be written:

|ε₂| = M|ΔI₁/Δt|

where:

  • ε₂ = induced EMF in Coil 2
  • M = mutual inductance
  • ΔI₁ = change in current in Coil 1
  • Δt = time interval

Including direction:

ε₂ = −M ΔI₁/Δt

The negative sign represents Lenz's law.


Meaning of Mutual Inductance

A large value of M means the coils are strongly coupled.

A relatively small change in primary current can produce a significant induced EMF in the second coil.

A small value of M means the coils are weakly coupled.

For the same rate of current change:

larger M → larger induced EMF


Meaning of One Henry

Suppose two coils have:

M = 1 H

If current in the first coil changes at:

1 A/s

the magnitude of the induced EMF in the second coil is:

1 V

Therefore:

1 H = 1 V·s/A

The henry is used for both:

  • self-inductance
  • mutual inductance

How Mutual Induction Occurs

Consider two nearby coils.

Coil 1 carries a changing current.

This changing current produces a changing magnetic field.

Some of that field passes through Coil 2.

Therefore, the magnetic flux through Coil 2 changes.

Faraday's law states:

ε = −N ΔΦ/Δt

so an EMF appears in Coil 2.

If Coil 2 forms part of a closed circuit, this EMF can produce a current.


EMF Does Not Always Mean Current

An important distinction is:

changing magnetic flux produces an EMF

but current flows only if there is a complete conducting path.

Therefore, an open secondary coil can have an induced voltage across its terminals even though no current flows.

If the secondary circuit is closed:

induced EMF → induced current


Energy Transfer Between Coils

Mutual inductance allows energy to move from one circuit to another through a magnetic field.

The basic energy pathway is:

electrical energy in Coil 1 → changing magnetic field → electrical energy in Coil 2

The coils do not need to touch.

They also do not need a direct electrical connection.

Instead, they must be magnetically coupled.

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10

Primary and Secondary Coils

In many mutual-induction systems, the coils are called:

Primary coil — receives the original electrical input.

Secondary coil — receives energy through electromagnetic induction.

The changing current in the primary creates the changing magnetic flux responsible for the induced EMF in the secondary.

These terms are especially common when discussing transformers.


Energy Is Conserved

Mutual inductance does not create energy.

Energy transferred to the secondary ultimately comes from the source connected to the primary.

For an ideal system:

input energy = output energy

and:

input power = output power

Real devices lose some energy through:

  • electrical resistance
  • eddy currents
  • magnetic hysteresis
  • flux leakage
  • heating

Therefore:

P_output < P_input

in real systems.


Why Changing Current Is Required

Suppose the primary carries a constant current.

A constant current produces a constant magnetic field.

A constant magnetic field produces constant magnetic flux through the secondary.

Therefore:

ΔΦ/Δt = 0

and:

ε₂ = 0

So a steady current does not produce continuous mutual induction.

What matters is:

changing current

rather than simply the presence of current.


Switching DC On and Off

A DC circuit can still produce mutual induction briefly.

When the primary is switched on:

  • current increases
  • magnetic field increases
  • secondary flux increases
  • EMF is induced

Once the current becomes steady:

induced EMF → 0

When the primary is switched off:

  • current decreases
  • magnetic field collapses
  • secondary flux decreases
  • another EMF is induced

The induced EMF during switch-off has the opposite direction from that during switch-on.


Alternating Current

Alternating current continually changes.

Therefore:

AC → changing magnetic field → changing magnetic flux → continuous induced EMF

This makes AC especially useful for devices based on mutual induction.

Transformers are the most important example.


Factors Affecting Mutual Inductance

Mutual inductance depends on how effectively the magnetic field from one coil links with the other.

Important factors include:

  • number of turns
  • distance between coils
  • orientation of coils
  • amount of overlap
  • coil size and geometry
  • magnetic core
  • magnetic permeability
  • leakage flux

Together, these determine the strength of magnetic coupling.


Number of Turns

Increasing the number of turns can increase mutual inductance.

More turns in the primary can strengthen its magnetic effect.

More turns in the secondary provide greater total flux linkage.

Therefore:

more turns → potentially greater mutual inductance

The exact relationship depends on the geometry of the two coils.


Distance Between the Coils

Mutual inductance generally becomes smaller as the coils are moved farther apart.

At greater distances:

  • less primary magnetic field reaches the secondary
  • less flux links the secondary
  • coupling becomes weaker

Therefore:

greater separation → smaller M

in typical arrangements.


Coil Orientation

The relative orientation of the coils is extremely important.

If the coils are aligned so that much of the primary field passes through the secondary:

mutual inductance is relatively large

If one coil is rotated:

  • less magnetic flux may pass through it
  • flux linkage decreases
  • mutual inductance decreases
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7

Why Orientation Matters

Magnetic flux is:

Φ = BA cos θ

where θ is the angle between the magnetic field and the normal to the coil.

When the magnetic field is perpendicular to the plane of the coil:

θ = 0°

and:

Φ = BA

The flux is maximum.

If the field lies parallel to the plane:

θ = 90°

and:

Φ = 0

Therefore, changing the orientation of the secondary can dramatically change the magnetic flux linking it.


Coil Overlap

Coils that strongly overlap can share more magnetic flux.

If the coils are moved sideways so that their overlap decreases, less magnetic flux may link them.

Therefore:

greater effective overlap → stronger coupling

This principle is important in wireless power-transfer systems.


Magnetic Cores

A suitable magnetic core can greatly increase mutual inductance.

The core provides a path that guides magnetic flux from one coil through the other.

This can:

  • increase magnetic flux
  • reduce leakage
  • improve coupling
  • increase mutual inductance
  • improve energy transfer

Transformer cores are designed for exactly this purpose.

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7

Flux Leakage

Not all magnetic flux produced by the primary necessarily passes through the secondary.

The portion that does not link effectively with the other coil is called leakage flux.

Greater leakage means:

  • weaker magnetic coupling
  • smaller mutual inductance
  • less effective energy transfer

Reducing leakage is therefore important when strong coupling is required.


Coupling Coefficient

The degree of magnetic coupling can also be described by the coupling coefficient, k.

For two coils:

M = k√(L₁L₂)

where:

  • M = mutual inductance
  • L₁ = self-inductance of Coil 1
  • L₂ = self-inductance of Coil 2
  • k = coupling coefficient

For idealized systems:

0 ≤ k ≤ 1


Meaning of the Coupling Coefficient

If:

k ≈ 1

the coils are very strongly coupled.

If:

k ≈ 0

the coils are very weakly coupled.

The equation:

M = k√(L₁L₂)

shows that mutual inductance depends on both:

  • the inductances of the individual coils
  • how effectively they are magnetically coupled

Worked Example: Coupling Coefficient

Two coils have:

L₁ = 4.0 H

L₂ = 9.0 H

and:

k = 0.50

Use:

M = k√(L₁L₂)

M = 0.50√[(4.0)(9.0)]

M = 0.50√36

M = 0.50(6.0)

M = 3.0 H


Worked Example: Induced EMF

Two coils have mutual inductance:

M = 0.40 H

The current in Coil 1 changes from:

2.0 A to 8.0 A

in:

0.30 s

Calculate:

ΔI₁ = 8.0 − 2.0

ΔI₁ = 6.0 A

Rate of current change:

ΔI₁/Δt = 6.0/0.30

ΔI₁/Δt = 20 A/s

Then:

|ε₂| = M|ΔI₁/Δt|

|ε₂| = (0.40)(20)

|ε₂| = 8.0 V


Worked Example: Finding Mutual Inductance

A changing current in Coil 1 produces an induced EMF of:

12 V

in Coil 2.

The current changes at:

30 A/s

Use:

|ε₂| = M|ΔI₁/Δt|

Rearrange:

M = |ε₂| / |ΔI₁/Δt|

M = 12/30

M = 0.40 H


Worked Example: Finding Rate of Current Change

Two coils have:

M = 0.25 H

The secondary experiences:

|ε₂| = 5.0 V

Use:

|ΔI₁/Δt| = |ε₂|/M

|ΔI₁/Δt| = 5.0/0.25

|ΔI₁/Δt| = 20 A/s


Self-Inductance

Self-inductance occurs when a changing current produces an induced EMF in the same circuit.

The relationship is:

ε = −L ΔI/Δt

where L is the self-inductance.

The coil responds to changes in its own current.


Mutual Inductance

Mutual inductance occurs when changing current in one circuit induces an EMF in another circuit.

The relationship is:

ε₂ = −M ΔI₁/Δt

where M is the mutual inductance.

The second coil responds to the changing magnetic field produced by the first.


Comparing Self-Inductance and Mutual Inductance

Self-Inductance Mutual Inductance
Occurs within the same circuit Occurs between two circuits
Uses L Uses M
ε = −L ΔI/Δt ε₂ = −M ΔI₁/Δt
Circuit responds to its own changing current Second circuit responds to changing current in first
Important in inductors and RL circuits Important in transformers and coupled coils
Measured in henries Measured in henries

Both are consequences of Faraday's law and Lenz's law.


Both Effects Can Occur Together

Suppose two coils are placed around the same magnetic core.

When current changes in Coil 1:

  • Coil 1 experiences self-induction
  • Coil 2 experiences mutual induction

Therefore, self-inductance and mutual inductance can occur simultaneously.

This happens in transformers.


Transformers

A transformer is one of the most important applications of mutual inductance.

It contains:

  • a primary winding
  • a secondary winding
  • usually a magnetic core

Alternating current in the primary produces a continuously changing magnetic field.

The core guides much of this changing magnetic flux through the secondary.

An alternating EMF is then induced in the secondary.

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8

Energy Transfer in a Transformer

The transformer energy pathway can be represented as:

electrical energy in primary

↓

changing magnetic field

↓

changing magnetic flux through secondary

↓

electrical energy in secondary

The windings can remain electrically isolated even though energy is transferred between them.


Transformer Voltage Ratio

For an ideal transformer:

V_s/V_p = N_s/N_p

where:

  • V_s = secondary voltage
  • V_p = primary voltage
  • N_s = number of secondary turns
  • N_p = number of primary turns

Changing the turns ratio allows the transformer to change voltage.


Step-Up Transformers

For a step-up transformer:

N_s > N_p

so:

V_s > V_p

The transformer increases voltage.

For an ideal transformer, this increase in voltage is accompanied by a decrease in current.


Step-Down Transformers

For a step-down transformer:

N_s < N_p

so:

V_s < V_p

The transformer decreases voltage.

For an ideal transformer, the secondary current can then be greater than the primary current.


Wireless Charging

Wireless charging is another important application of mutual inductance.

A transmitter coil carries alternating current.

This creates a changing magnetic field.

A receiver coil inside the device experiences changing magnetic flux.

An EMF is induced in the receiver.

The resulting electrical energy can be used to charge a battery.

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9

Why Wireless Charger Position Matters

If the transmitter and receiver coils are well aligned:

  • magnetic coupling is stronger
  • mutual inductance is greater
  • more flux links the receiver

If the device is badly aligned:

  • coupling becomes weaker
  • less flux links the receiver
  • energy transfer becomes less effective

This is why the position of a device on a wireless charging pad matters.


Electric Toothbrush Charging

Inductive charging is useful in devices where exposed electrical contacts may be undesirable.

Some electric toothbrush chargers contain:

  • a transmitting coil in the base
  • a receiving coil in the toothbrush

Changing current in the base produces a changing magnetic field.

Mutual induction transfers energy to the toothbrush without requiring exposed electrical contacts between the charger and device.


Inductive Sensors

Mutual inductance is also used in sensing systems.

A changing magnetic field produced by one coil can interact with:

  • another coil
  • conducting objects
  • magnetic materials

Changes in coupling can then be detected electrically.

Applications include:

  • position sensors
  • proximity sensors
  • metal detectors
  • industrial measurement systems

Signal Transfer

Mutual inductance can transfer changing electrical signals between circuits.

Small transformers are used in some electronic systems for:

  • signal coupling
  • electrical isolation
  • impedance matching
  • noise control

The circuits can exchange energy and information without sharing a direct conductive path.


Ignition Systems

Some ignition systems use strongly coupled coils.

Energy is first stored in a magnetic field.

When current changes rapidly, a large change in magnetic flux occurs.

A secondary winding with many turns can develop a very large voltage.

This high voltage can then be used to create an electrical spark.


Electrical Isolation

Transformers can provide galvanic isolation.

The primary and secondary may have no direct conducting connection.

Instead:

energy crosses through magnetic coupling

This can help:

  • improve safety
  • isolate sensitive circuits
  • reduce unwanted ground connections
  • protect equipment

Strong and Weak Coupling

Consider two identical pairs of coils.

System A

The coils are:

  • close together
  • aligned
  • wrapped around the same magnetic core

This system has relatively strong coupling and high mutual inductance.

System B

The coils are:

  • far apart
  • poorly aligned
  • surrounded mainly by air

This system has much weaker coupling and lower mutual inductance.


Comparing Coil Arrangements

Suppose the same changing primary current is applied to several arrangements.

The largest induced secondary voltage would generally occur when the coils have:

  • many turns
  • close spacing
  • strong alignment
  • large useful overlap
  • a suitable shared magnetic core

The smallest induced voltage would generally occur when the coils are:

  • far apart
  • poorly aligned
  • weakly coupled

Energy Transfer Efficiency

Strong mutual inductance does not automatically mean a device is perfectly efficient.

Real systems can lose energy because of:

  • wire resistance
  • eddy-current heating
  • hysteresis
  • leakage flux
  • electromagnetic radiation
  • other circuit losses

Designers therefore try to achieve strong useful coupling while minimizing losses.


Mutual Inductance and Eddy Currents

Mutual induction involves intended coupling between circuits or coils.

However, changing magnetic fields can also induce unwanted circulating currents in nearby conducting materials.

These are eddy currents.

For example, transformer cores can develop eddy currents.

Laminated cores help reduce these unwanted currents and their associated heating.


Mutual Inductance and RL Circuits

The primary winding of a transformer has self-inductance.

Therefore, its current does not necessarily change instantaneously.

At the same time, its changing magnetic field can induce an EMF in another winding.

So the concepts studied in:

  • self-induction
  • inductance
  • RL circuits
  • magnetic energy
  • mutual induction

are closely connected.


A Complete Calculation

Two coils have:

M = 0.60 H

The primary current decreases from:

8.0 A to 2.0 A

in:

0.20 s

Change in current:

ΔI₁ = 2.0 − 8.0

ΔI₁ = −6.0 A

Magnitude of the rate:

|ΔI₁/Δt| = 6.0/0.20

|ΔI₁/Δt| = 30 A/s

Induced EMF:

|ε₂| = M|ΔI₁/Δt|

|ε₂| = (0.60)(30)

|ε₂| = 18 V

The induced effect acts according to Lenz's law to oppose the decrease in magnetic flux.


Complete Coupling Problem

Two coils have:

L₁ = 0.80 H

L₂ = 0.20 H

and coupling coefficient:

k = 0.75

Calculate their mutual inductance.

Use:

M = k√(L₁L₂)

M = 0.75√[(0.80)(0.20)]

M = 0.75√0.16

M = 0.75(0.40)

M = 0.30 H

If current in Coil 1 changes at:

10 A/s

then:

|ε₂| = M|ΔI₁/Δt|

|ε₂| = (0.30)(10)

|ε₂| = 3.0 V


A Reliable Strategy for Mutual-Inductance Problems

First identify:

  • which coil has the changing current
  • which coil experiences the induced EMF
  • whether the coils are magnetically coupled

For a simple induced-EMF problem use:

|ε₂| = M|ΔI₁/Δt|

For coupling problems use:

M = k√(L₁L₂)

For transformer problems, the turns ratio may be needed:

V_s/V_p = N_s/N_p

Then consider the physical arrangement:

  • distance
  • orientation
  • turns
  • core material
  • overlap
  • leakage flux

Finally, use Lenz's law if the direction of the induced effect is required.


Common Mistakes

Confusing mutual inductance with mutual induction

Mutual induction is the process. Mutual inductance M is the quantity describing the strength of coupling.

Thinking the coils must be electrically connected

They can transfer energy magnetically while remaining electrically isolated.

Thinking a steady current continuously induces an EMF

A steady current produces a steady field. Continuous induction requires changing magnetic flux.

Ignoring coil position

Distance and orientation strongly affect coupling.

Assuming all magnetic flux links both coils

Some flux can leak away.

Confusing L and M

L describes self-inductance. M describes mutual inductance.

Forgetting the rate of current change

Induced EMF depends on ΔI/Δt, not simply the amount of current.

Assuming energy is created in the secondary

Energy transferred to the secondary ultimately comes from the primary circuit.

Thinking stronger coupling means perfect efficiency

Resistance, core losses, leakage, and other effects can still reduce efficiency.


Key Terms

Mutual inductance — measure of how strongly changing current in one circuit induces an EMF in another circuit.

Mutual induction — process by which changing current in one circuit produces an induced EMF in another.

Self-inductance — ability of a circuit's changing current to induce an EMF in the same circuit.

Henry (H) — SI unit of self-inductance and mutual inductance.

Primary coil — coil carrying the changing current that produces the changing magnetic field.

Secondary coil — coil in which an EMF is induced by changing magnetic flux from another coil.

Magnetic coupling — degree to which magnetic flux produced by one circuit links another circuit.

Coupling coefficient — number k describing the strength of magnetic coupling between two inductors.

Flux linkage — total magnetic flux linked with the turns of a coil.

Leakage flux — magnetic flux that does not effectively link both coupled coils.

Faraday's law — relationship between changing magnetic flux and induced EMF.

Lenz's law — principle stating that an induced effect opposes the change producing it.

Transformer — device that transfers electrical energy between circuits using mutual induction.

Galvanic isolation — separation of circuits so there is no direct conductive connection between them.

Wireless power transfer — transfer of electrical energy without direct electrical contacts, often using magnetic coupling.


Key Takeaways

  • Mutual inductance describes electromagnetic coupling between two circuits.
  • Its symbol is M and its SI unit is the henry.
  • Changing current in one coil produces a changing magnetic field.
  • Changing magnetic flux through another coil produces an induced EMF.
  • For simple situations, |ε₂| = M|ΔI₁/Δt|.
  • Faster current changes produce larger induced EMFs.
  • Greater mutual inductance produces larger induced EMFs for the same rate of current change.
  • Mutual induction transfers energy through magnetic fields rather than through a direct electrical connection.
  • A secondary circuit must be closed for an induced current to flow, although an induced EMF can exist in an open circuit.
  • Mutual inductance depends on coil geometry, turns, distance, orientation, overlap, and core material.
  • Moving coils closer together generally increases coupling.
  • Better coil alignment generally increases coupling.
  • A suitable common magnetic core can greatly increase mutual inductance.
  • Leakage flux reduces magnetic coupling.
  • The coupling coefficient can be used with M = k√(L₁L₂).
  • Self-inductance involves one circuit responding to its own changing current.
  • Mutual inductance involves one circuit responding to changing current in another circuit.
  • Both self-inductance and mutual inductance follow Faraday's and Lenz's laws.
  • Transformers use mutual inductance to transfer electrical energy between windings.
  • Wireless chargers use magnetic coupling between transmitter and receiver coils.
  • Mutual inductance is also important in sensors, ignition systems, signal transformers, and electrically isolated circuits.

Check Your Understanding

  1. Define mutual inductance and state its SI unit.
  2. Explain the difference between mutual induction and mutual inductance.
  3. Describe how changing current in one coil can produce an EMF in another coil.
  4. Why does a constant DC current in the primary not continuously induce an EMF in the secondary?
  5. Explain how energy can be transferred between two coils that have no direct electrical connection.
  6. Identify four factors that can affect mutual inductance between two coils.
  7. Explain why moving two coils farther apart generally decreases their mutual inductance.
  8. Explain why changing the orientation of one coil can affect the induced EMF.
  9. Two coils have M = 0.30 H. Current in Coil 1 changes at 20 A/s. Calculate the magnitude of the induced EMF in Coil 2.
  10. A secondary coil experiences an induced EMF of 12 V when primary current changes at 40 A/s. Calculate the mutual inductance.
  11. Two coils have L₁ = 2.0 H, L₂ = 8.0 H, and k = 0.50. Calculate their mutual inductance.
  12. Compare self-inductance and mutual inductance. Give at least two similarities and two differences.
  13. Explain how mutual inductance allows a transformer to transfer electrical energy from its primary winding to its secondary winding.
  14. Explain why correct alignment between transmitter and receiver coils is important in a wireless charging system.
  15. An engineer wants to increase the mutual inductance between two coils. Describe at least four changes that could be made to their design or arrangement and explain why each would help.

5. Practical Inductance Applications

Learning outcomes
  • I can identify devices that use inductors.
  • I can explain the role of inductors in electrical circuits.
  • I can describe how inductors reduce electrical noise.
  • I can explain how inductors are used in power supplies.
  • I can evaluate the advantages of inductors in modern electronics.

Practical Inductance Applications

Inductors are used throughout modern electrical and electronic systems because they oppose rapid changes in current and store energy in magnetic fields.

An inductor is usually made from a coil of conducting wire. Many inductors also contain a magnetic core to increase their inductance.

Their behaviour is based on self-induction:

changing current → changing magnetic field → self-induced EMF

The induced EMF opposes the change in current according to Lenz's law.

This simple effect allows inductors to perform several important jobs:

  • storing and transferring energy
  • smoothing changing currents
  • reducing electrical noise
  • filtering signals
  • converting voltages efficiently
  • controlling current in motors and other devices
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6

Inductors in Everyday Electronics

Inductors are found in many familiar devices, including:

  • phone chargers
  • laptop power supplies
  • televisions
  • radios
  • computers
  • Wi-Fi equipment
  • LED lighting
  • electric vehicles
  • electric motors
  • audio equipment
  • solar power systems

Some inductors are large coils that are easy to recognize.

Others are extremely small components mounted directly onto circuit boards.


Why Inductors Are Useful

The key property of an inductor is that it opposes changes in current.

The induced EMF is related to:

|ε| = L|ΔI/Δt|

where:

  • ε = induced EMF
  • L = inductance
  • ΔI/Δt = rate of current change

Rapid current changes therefore produce larger inductive effects.

This makes inductors particularly useful in circuits containing rapidly changing or switching currents.


Inductors and Steady DC

An ideal inductor behaves differently depending on whether the current is changing.

When DC current is changing:

  • the magnetic field changes
  • self-induced EMF occurs
  • the inductor opposes the current change

When the current becomes steady:

ΔI/Δt = 0

so:

ε = 0

An ideal inductor therefore has zero induced voltage once steady DC conditions are reached.

A real inductor still has some resistance in its wire.


Energy Storage

An inductor stores energy in its magnetic field.

The stored energy is:

E = ½LI²

where:

  • E = energy in joules
  • L = inductance in henries
  • I = current in amperes

When current increases, magnetic energy increases.

When current decreases, the magnetic field can return energy to the circuit.

This temporary energy storage is extremely important in modern power electronics.


Inductors in Power Supplies

One of the most important applications of inductors is in power supplies.

Electronic devices often require a different voltage from the available power source.

For example:

  • a battery voltage may need to be reduced
  • a battery voltage may need to be increased
  • an AC supply may need to be converted to controlled DC
  • a varying input may need to produce a stable output

Inductors help accomplish these tasks efficiently.

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8

Switching Power Supplies

Modern electronics commonly use switch-mode power supplies.

Instead of continuously wasting excess electrical energy as heat, electronic switches turn on and off rapidly.

Inductors repeatedly:

store magnetic energy → release magnetic energy

during each switching cycle.

This allows electrical energy to be transferred and converted efficiently.


Why Switching Works

Imagine a switch connected to an inductor.

When the switch is turned on:

  • current increases
  • magnetic field strengthens
  • energy is stored

When the circuit switches configuration:

  • current begins changing
  • magnetic field changes
  • the inductor produces an induced voltage
  • stored energy is transferred elsewhere in the circuit

This process may occur thousands or millions of times each second in modern electronics.


Buck Converters

A buck converter reduces DC voltage.

For example, a circuit might convert:

12 V → 5 V

The inductor helps maintain a relatively smooth output current while an electronic switch rapidly turns on and off.

During part of the switching cycle, energy is stored in the magnetic field.

During another part, the stored energy is delivered to the load.

This allows efficient voltage reduction.


Boost Converters

A boost converter increases DC voltage.

For example:

5 V → 12 V

During one part of the cycle:

  • current increases through the inductor
  • magnetic energy is stored

During another part:

  • the magnetic field collapses
  • the inductor produces an induced voltage
  • its voltage contributes to the output

This can produce an output voltage greater than the input voltage.


Buck-Boost Converters

A buck-boost converter can increase or decrease voltage depending on its design and operating conditions.

Inductive energy storage allows energy to be transferred between different parts of the circuit.

Buck-boost systems are useful when battery voltage changes during operation but the electronics require a controlled output.


Phone and Laptop Chargers

Modern chargers commonly contain inductive components as part of their switching power supplies.

Their functions can include:

  • temporary energy storage
  • voltage conversion
  • current smoothing
  • noise filtering
  • electromagnetic interference reduction

Efficient switching designs allow chargers to be much smaller than older power supplies while still handling significant electrical power.


Smoothing Current

Switching circuits naturally produce rapid variations in current.

Many electronic devices require a much smoother electrical supply.

An inductor resists rapid current changes.

Therefore, it can reduce the size of these fluctuations.

The result is:

rapidly varying current → inductor → smoother current

This is often called current smoothing.


Current Ripple

Small repeated variations around the desired current are often called ripple.

For example, instead of remaining perfectly constant, current might repeatedly rise and fall slightly.

An inductor helps reduce current ripple because:

rapid current change → larger self-induced EMF

The inductor therefore opposes the rapid increase and decrease.


Inductors as Electrical Filters

Inductors can also help separate unwanted high-frequency signals from useful lower-frequency signals.

For sinusoidal AC, the opposition provided by an ideal inductor is described by inductive reactance:

X_L = 2πfL

where:

  • X_L = inductive reactance in ohms
  • f = frequency in hertz
  • L = inductance in henries

As frequency increases:

X_L increases

Therefore, an inductor has a stronger effect on higher-frequency current variations.


Worked Example: Inductive Reactance

An inductor has:

L = 0.020 H

At:

f = 50 Hz

X_L = 2πfL

X_L = 2π(50)(0.020)

X_L ≈ 6.3 Ω

At:

f = 5000 Hz

X_L = 2π(5000)(0.020)

X_L ≈ 628 Ω

The same inductor provides much greater opposition to the higher-frequency signal.


Reducing Electrical Noise

Electronic circuits can contain unwanted rapidly changing signals called electrical noise.

Noise can come from:

  • switching circuits
  • motors
  • radio-frequency signals
  • digital electronics
  • power lines
  • nearby electronic equipment

Because many forms of unwanted noise contain high-frequency components, inductors can help reduce them.

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9

Chokes

An inductor designed mainly to reduce unwanted AC or high-frequency signals is often called a choke.

A choke can allow desired DC current to pass while providing greater opposition to rapidly changing current.

Therefore:

desired DC → passes relatively easily

while:

high-frequency noise → strongly opposed

Chokes are widely used in power supplies and communication equipment.


Filtering Power-Supply Noise

A DC power supply may contain:

  • useful DC
  • unwanted AC ripple
  • high-frequency switching noise

An inductor can help separate these components.

The DC component is steady and therefore produces little inductive opposition.

Rapid variations produce larger inductive effects.

This allows an inductor to help create a cleaner DC supply.


Inductors and Capacitors Together

Inductors are often combined with capacitors.

They have complementary behaviour:

Inductor: opposes rapid changes in current.

Capacitor: opposes rapid changes in voltage.

Together, they can form powerful filtering circuits.

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8

LC Filters

An LC filter contains:

  • an inductor, L
  • a capacitor, C

The inductor helps smooth current.

The capacitor helps smooth voltage.

Together, they can reduce unwanted variations more effectively than either component alone.

LC filters are common in:

  • power supplies
  • audio systems
  • radio circuits
  • communication equipment
  • motor controllers

Common-Mode Chokes

Some cables carry unwanted high-frequency noise that appears in similar ways on multiple conductors.

A common-mode choke uses coupled windings to strongly oppose this unwanted noise while allowing the intended current or signal to pass.

Common-mode chokes are often found in:

  • computer equipment
  • power adapters
  • communication systems
  • USB and other data interfaces
  • industrial electronics

They help reduce electromagnetic interference (EMI).


Electromagnetic Interference

Electromagnetic interference, or EMI, is unwanted electromagnetic energy that interferes with the operation of electrical equipment.

EMI can cause:

  • distorted signals
  • communication errors
  • audio noise
  • unstable electronics
  • interference with nearby devices

Inductive filters help prevent unwanted high-frequency currents from travelling through wires and cables.


Ferrite Components

Ferrite is a magnetic ceramic material commonly used in high-frequency inductive components.

You may have seen a cylindrical or enlarged section near the end of a computer or display cable.

Some of these devices contain ferrite material that helps reduce high-frequency interference.

Ferrite components are useful because they can provide strong magnetic effects while limiting unwanted eddy-current losses at high frequencies.

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7

Inductors in Radio Circuits

Inductors are important in radio-frequency circuits.

When combined with capacitors, they can form resonant circuits that respond strongly to particular frequencies.

This allows circuits to:

  • select radio frequencies
  • reject unwanted frequencies
  • tune transmitters
  • tune receivers
  • filter communication signals

The ability to select frequencies is fundamental to radio and wireless communication.


LC Resonance

In an LC circuit, energy can move between:

  • the capacitor's electric field
  • the inductor's magnetic field

The capacitor stores energy as:

E_C = ½CV²

The inductor stores energy as:

E_L = ½LI²

This exchange can produce electrical oscillations.

The resonant frequency of an ideal LC circuit is:

f = 1/(2π√(LC))


Example: Radio Tuning

Suppose a radio receives many frequencies simultaneously.

A carefully chosen combination of L and C can have a resonant frequency corresponding to the desired station.

The circuit responds strongly near that frequency while responding less strongly to many other frequencies.

Changing L or C changes the resonant frequency.

This allows the circuit to be tuned.


Inductors in Audio Systems

Inductors can also be used in audio crossover networks.

Different speakers are designed for different frequency ranges.

For example:

  • woofers reproduce lower frequencies
  • tweeters reproduce higher frequencies

Inductors and capacitors can help direct appropriate frequency ranges to different speakers.


Inductors in Electric Motors

Motor windings are coils and therefore have inductance.

Their inductance affects:

  • how quickly current changes
  • motor starting behaviour
  • current ripple
  • electromagnetic torque
  • electronic motor control

Modern motor controllers must account for the inductance of the motor windings.


Motor Current Smoothing

Electronic motor controllers often switch voltage rapidly.

Without inductance, current could change very rapidly.

Motor winding inductance helps smooth these changes.

This is especially important in:

  • electric vehicles
  • drones
  • robots
  • industrial machines
  • computer cooling fans

Relays and Solenoids

Relays and electromagnetic solenoids contain coils.

When current flows:

  • a magnetic field develops
  • magnetic energy is stored
  • magnetic forces can move mechanical components

Examples include:

  • electrical switches
  • valves
  • door locks
  • automotive actuators

Because these coils have inductance, switching them off can produce large induced voltages.


Flyback Protection

When current through a coil is suddenly interrupted:

|ε| = L|ΔI/Δt|

If Δt is very small, the induced voltage can become very large.

A flyback diode can provide a temporary path for current when a DC inductive load is switched off.

The stored magnetic energy is then released more safely.

This protects components such as transistors and switches.

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7

Transformers

Transformers contain inductive windings.

Alternating current in the primary produces changing magnetic flux.

Mutual induction produces an EMF in the secondary.

Transformers can:

  • increase voltage
  • decrease voltage
  • provide electrical isolation
  • transfer signals
  • transfer electrical power

Inductance is therefore central to transformer operation.


Wireless Charging

Wireless charging also uses inductive effects.

An alternating current passes through a transmitter coil.

The changing magnetic field reaches a receiver coil.

Mutual induction produces an EMF in the receiver.

Energy can therefore be transferred without exposed electrical contacts.

Applications include:

  • smartphones
  • smartwatches
  • electric toothbrushes
  • some medical devices
  • some electric vehicle charging systems

Inductive Sensors

Inductors can be used as sensors because nearby materials can affect their magnetic fields.

Applications include:

  • proximity sensors
  • position sensors
  • metal detectors
  • vehicle detection systems
  • industrial automation

A nearby conducting or magnetic object changes the electromagnetic behaviour of the sensor coil, allowing the electronics to detect its presence.


Induction Heating

Changing magnetic fields can induce currents in nearby conducting materials.

These currents can produce heating.

Induction heating is used in:

  • induction cooktops
  • industrial metal heating
  • metal treatment
  • manufacturing

The coil itself creates the changing magnetic field responsible for the induction process.


Energy Storage in Power Electronics

Inductors are particularly useful because they can store and release energy extremely quickly.

Suppose an inductor has:

L = 0.50 H

and carries:

I = 4.0 A

Stored energy:

E = ½LI²

E = ½(0.50)(4.0²)

E = 4.0 J

If current changes, this energy can be transferred elsewhere in the circuit.


Worked Example: Power-Supply Inductor

A power-supply inductor has:

L = 5.0 mH

and carries:

I = 3.0 A

Convert:

5.0 mH = 0.0050 H

Then:

E = ½LI²

E = ½(0.0050)(3.0²)

E = 0.0025(9)

E = 0.0225 J

Although this is a relatively small amount of energy, the inductor may store and release energy thousands of times per second.

The rate of energy transfer can therefore be significant.


Advantages of Inductors

Inductors provide several important advantages.

They can:

  • store energy without relying on chemical reactions
  • release stored energy very rapidly
  • smooth current
  • reduce ripple
  • suppress high-frequency noise
  • help filter signals
  • enable efficient switching power supplies
  • support voltage conversion
  • provide frequency selection
  • operate reliably for very large numbers of cycles

These properties make them extremely valuable in modern electronics.


High Efficiency

An ideal inductor does not dissipate energy.

Instead:

electrical energy → magnetic energy → electrical energy

Real inductors do have losses, but efficient designs can transfer a large fraction of their stored energy back into the circuit.

This makes inductors particularly useful in efficient power-conversion systems.


Fast Response

Magnetic energy can be stored and released quickly.

Unlike chemical energy storage, no chemical reaction is required.

This makes inductors suitable for circuits switching at high frequencies.

Modern power converters can therefore repeatedly store and release energy many thousands or millions of times per second.


Reliability

Inductors are often simple components with no moving parts.

This can provide:

  • long operating life
  • high reliability
  • large numbers of operating cycles

This is especially useful in power electronics and industrial equipment.


Limitations of Inductors

Inductors also have disadvantages.

Real inductors can:

  • occupy significant circuit-board space
  • be relatively heavy
  • have wire resistance
  • generate heat
  • produce electromagnetic interference
  • experience magnetic-core losses
  • saturate at high currents
  • be more expensive than simple resistors

Engineering design involves balancing these disadvantages against the benefits.


Copper Losses

The wire used to make an inductor has resistance.

Therefore:

P = I²R

describes power converted into thermal energy in the winding.

Large currents can therefore cause significant heating.

Using lower-resistance conductors can reduce these losses.


Core Losses

Magnetic cores can experience energy losses.

Two important mechanisms are:

  • eddy currents
  • magnetic hysteresis

Core materials and construction are selected to reduce these effects.

For example:

  • laminated cores can reduce eddy currents
  • ferrite materials are useful at higher frequencies

Magnetic Saturation

Magnetic cores cannot always respond proportionally to indefinitely increasing current.

At sufficiently strong magnetic fields, a core may approach magnetic saturation.

When this occurs:

  • effective inductance can decrease
  • current may increase rapidly
  • losses and heating can increase
  • circuit performance may deteriorate

Engineers therefore choose inductors with suitable current ratings.


Size and Energy Storage

Storing significant magnetic energy generally requires:

  • sufficient inductance
  • sufficient current capability
  • adequate magnetic core volume
  • suitable conductor size

This is one reason high-power inductors can be physically large.

Miniaturizing inductors while maintaining efficiency and current capacity is an important engineering challenge.


Inductors vs Resistors

Inductor Resistor
Stores magnetic energy Mainly dissipates energy as heat
Opposes changes in current Opposes current
Ideal component can return stored energy Does not return dissipated thermal energy
Frequency-dependent behaviour Ideal resistance largely frequency-independent
Important in filters and power conversion Important in current and voltage control

Inductors vs Capacitors

Inductor Capacitor
Stores magnetic field energy Stores electric field energy
Energy = ½LI² Energy = ½CV²
Opposes rapid current changes Opposes rapid voltage changes
Current cannot change instantly in ideal model Voltage cannot change instantly in ideal model
Useful for current smoothing Useful for voltage smoothing

Inductors and capacitors are often used together because their properties complement each other.


Choosing an Inductor

Engineers may consider:

  • inductance
  • maximum current
  • resistance
  • core material
  • physical size
  • operating frequency
  • saturation current
  • energy-storage capacity
  • heat generation
  • electromagnetic interference

The "largest inductance" is therefore not automatically the best choice.

A successful design balances several requirements.


Evaluating Inductors in Modern Electronics

Inductors remain extremely useful because modern electronics increasingly relies on rapid switching.

Switching is used to control energy efficiently rather than continuously dissipating excess energy.

Inductors are well suited to this because they can:

store energy during one part of a switching cycle

and:

release energy during another part

This allows efficient control of electrical power.


Electric Vehicles

Electric vehicles contain numerous inductive components.

They can appear in:

  • motor windings
  • DC-DC converters
  • onboard chargers
  • electromagnetic interference filters
  • power-conditioning systems

Inductance helps control the very large electrical currents involved in vehicle operation.


Renewable Energy

Solar panels and wind turbines often produce electrical power that must be converted before it can be used or supplied to a grid.

Power-electronic converters use inductors to:

  • store energy temporarily
  • smooth current
  • filter switching noise
  • control power flow

Inductors therefore contribute to efficient renewable-energy systems.


Computers and Digital Electronics

Computer processors and other digital components can require low voltages and very large currents.

Voltage-regulator circuits commonly use inductors to convert and control electrical power efficiently.

You may see several small power inductors close to a computer processor or graphics chip.

Their job includes helping deliver stable power despite rapidly changing electrical demand.

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7

A Complete Application Example

Consider a computer power circuit that must convert:

12 V → lower controlled voltage

for a processor.

A switching transistor rapidly connects and disconnects the input.

The inductor:

  • stores magnetic energy when current increases
  • opposes sudden current changes
  • releases energy when the switching state changes
  • helps maintain continuous current
  • reduces current ripple

A capacitor can simultaneously help stabilize voltage.

Together, the switching components, inductor, and capacitor provide efficient power conversion.


Common Mistakes

Thinking inductors simply block electricity

Inductors oppose changes in current, not current itself.

Thinking an inductor always has a large voltage across it

The induced voltage depends on how rapidly the current changes.

Thinking inductors only work with AC

Inductors also affect DC circuits whenever the DC current changes, such as during switching.

Thinking inductors destroy unwanted electrical energy

Filtering often redirects, stores, releases, or dissipates unwanted variations through a combination of circuit components.

Thinking all noise has the same frequency

Electrical noise can contain many different frequencies, so filters must be designed for the particular application.

Thinking an ideal inductor consumes power continuously

An ideal inductor stores and returns energy. Real inductors have resistance and other losses.

Ignoring saturation

Real magnetic cores have limits to how strongly they can be magnetized.

Thinking larger inductance is always better

Greater inductance may also mean greater size, resistance, cost, or slower current response.


Key Terms

Inductor — component that stores energy in a magnetic field and opposes changes in current.

Inductance — measure of the ability of a circuit to produce self-induced EMF when current changes.

Self-induction — production of an induced EMF caused by a circuit's own changing current.

Magnetic energy — energy associated with the magnetic field of an inductor.

Switch-mode power supply — power supply that uses rapid electronic switching to control and convert electrical energy efficiently.

Buck converter — circuit that reduces DC voltage using switching and energy-storage components.

Boost converter — circuit that increases DC voltage using switching and energy-storage components.

Buck-boost converter — switching converter capable of producing an output voltage above or below its input under appropriate operation.

Ripple — unwanted repeated variation in voltage or current.

Choke — inductor designed to oppose unwanted changing currents or high-frequency signals.

Inductive reactance — opposition an ideal inductor provides to sinusoidal alternating current, given by X_L = 2πfL.

Electrical noise — unwanted electrical variations that interfere with desired signals or power.

Electromagnetic interference (EMI) — unwanted electromagnetic disturbance affecting electrical equipment.

LC filter — filter containing an inductor and capacitor.

Ferrite — magnetic ceramic material commonly used in high-frequency inductive components.

Magnetic saturation — condition in which a magnetic core can no longer respond proportionally to increasing magnetizing influence.

Flyback diode — component used to provide a safe current path when a DC inductive load is switched off.


Key Takeaways

  • Inductors are used extensively in modern electrical and electronic devices.
  • Their key property is opposition to changes in current.
  • Changing current produces self-induced EMF.
  • Inductors store energy in magnetic fields.
  • Stored magnetic energy is given by E = ½LI².
  • Inductors can store and release energy repeatedly and rapidly.
  • Switching power supplies use inductors for efficient energy transfer.
  • Buck converters use inductors while reducing DC voltage.
  • Boost converters use inductors while increasing DC voltage.
  • Inductors help smooth current and reduce ripple.
  • High-frequency signals experience greater inductive reactance because X_L = 2πfL.
  • Chokes use inductance to suppress unwanted changing currents and electrical noise.
  • Inductors and capacitors are frequently combined to form filters.
  • Common-mode chokes can help reduce electromagnetic interference.
  • Inductors are important in radios, audio systems, motors, transformers, sensors, wireless chargers, and power converters.
  • Motor windings and electromagnetic coils naturally possess inductance.
  • Real inductors experience resistance, heating, core losses, and possible saturation.
  • Inductors can improve efficiency because energy can be temporarily stored rather than simply dissipated.
  • Their disadvantages can include size, weight, resistance, cost, and magnetic interference.
  • Modern electronics depends heavily on inductors for efficient power conversion, current control, noise suppression, and signal filtering.

Check Your Understanding

  1. Identify five common devices or systems that use inductors.
  2. Explain why an inductor opposes rapid changes in current.
  3. Explain how an inductor can store energy and later return it to a circuit.
  4. Why can an inductor allow steady DC while strongly opposing high-frequency current variations?
  5. Calculate the inductive reactance of a 0.050 H inductor at 60 Hz.
  6. The same 0.050 H inductor is used at 6000 Hz. Calculate its inductive reactance and compare it with your answer to Question 5.
  7. Explain how an inductor can help reduce high-frequency electrical noise.
  8. What is a choke, and why is it useful in electronic equipment?
  9. Explain why inductors and capacitors are often used together in power-supply filters.
  10. Describe the role of an inductor in a buck converter.
  11. Describe how magnetic energy stored in an inductor can help a boost converter produce a higher output voltage.
  12. A 20 mH power inductor carries 5.0 A. Calculate the energy stored in its magnetic field.
  13. Explain why switching off a relay or solenoid can produce a large voltage and how a flyback diode can help protect the circuit.
  14. Evaluate two advantages and two disadvantages of using inductors in modern electronic devices.
  15. A designer needs a circuit that efficiently converts voltage, reduces current ripple, and suppresses high-frequency noise. Explain why inductors would be useful and identify other components that could be combined with them.