# What is Electromagnetic Induction?

## Principles and Worked Examples

Electromagnetic (EM) induction occurs when an electromagnetic field (emf) is induced in a wire, or more precisely when a complete loop of wire cuts across lines of a magnetic field; the movement induces a current and therefore an emf.

The emf can be increased by moving the wire faster, using a stronger magnet and making wires into a coil and ensuring that the wires cut across the field at 90 degrees.

The direction of the current induced is dependant on the direction of the magnetic field.

**A current carrying wire**

We can determine the direction of the field using the Right hand ‘screw’ rule for B field around a current carrying wire. The thumb represents the direction of the current and the fingers curve to follow the direction of the magnetic field.

**A Solenoid**

Solenoid Poles

The poles of a solenoid can be determined using the right hand screw rule and knowing that field lines always come out of the north pole and into the south.

Magnetic field

When drawing the magnetic field lines around a solenoid the crosses represent wires going into the page and the dots out of the page.

A magnetic field will also change the direction of a moving charge.

Moving Charge

When a charge moves through a magnetic field we are able to define conventional current and when the charge is confined within a wire a potential difference is induced and electrons will flow in a complete circuit**.**

## Faraday and Lenz’s Law

**There are two main laws relating to Magnetism**

**Lenz’s law **= “the direction of the induced current is always such that it opposes the change that causes the current”.

**Faraday’s law** = “the induced emf in a circuit is equal to the rate of change of magnetic flux linkage through the circuit”.

## Lenz’s Law

When a bar magnet is pushed into a coil of wire, an ammeter will show a reading, and when pulled out the meter deflects in the opposite direction. The induced current passing round the circuit creates a magnetic field around the coil.

Coil Field

The coil field must oppose the incoming north pole otherwise it would pull the north pole in faster;

- As the magnet enters the coil, the top of the coil becomes a north pole, this magnetic field will oppose the movement of the bar magnet.
- As the magnet leaves, the south pole will induce a north pole in the bottom of the coil

## Magnetic Flux and Linkage

Flux linkage is the linking of the magnetic field with the conductors of a coil when the magnetic field passes through the loops of the coil, expressed as a value. The flux linkage of a coil is simply the alternative term for the total flux, used for convenience in engineering.

Magnetic flux, Φ, is defined as:

The unit of Magnetic Flux is the Weber. Where ‘A’ is the area swept out = lΔs. The Magnetic Flux linkage through a coil of N turns is:

When the magnetic field is at an angle the equation becomes:

**ФN = NBA cos θ**

Where

- B =magnetic field, in Tesla (T)
- A = cross sectional area, in metres squared (m^2)
- N = number of coils

Since emf is the rate of change of magnetic flux x number of coils of wire, we get Lenz’s Law

**Example.** Calculate the magnitude of the induced emf when the magnet is thrust into the coil, given the following information: the single loop coil has a radius of 6.00 cm and the average value of B cosθ (this is given, since the bar magnet’s field is complex) increases from 0.0500 T to 0.250 T in 0.100 s.

**Solution:** To find the *magnitude* of emf, we use Faraday’s law of induction as stated by Emf = − NΔϕ Δt but without the minus sign that indicates direction: emf = N Δϕ Δt We are given that N=1 and Δt = 0.100s but we must determine the change in flux Δϕ before we can find emf. Since the area of the loop is fixed, we see that Δϕ = Δ(BA cosθ) = Δϕ = AΔ(B cosθ) Now Δ(B cosθ) = 0.200T, since it was given that B cosθ changes from 0.0500 to 0.250 T. The area of the loop is A = πr^2 = (3.14…)(0.060m)^2 = 1.13×10^−2 m^2 Thus, Δϕ = (1.13×10^−2 m^2)(0.200T) Entering the determined values into the expression for emf gives Emf = N Δϕ = (1.13×10^−2 m^2)(0.200T) = 22.6mV Δt 0.100s

## Dropping a Magnet into a Coil

Moving Magnet

- As the magnet enters, it induces a current in the loop that sets up a magnetic field to oppose the entry of the magnet
- When the magnet is in the middle of the coil it is at the point where the magnetic poles will switch. At this point there is no current flowing in the coil since the p.d is zero.
- When exiting the coil, the magnet is moving faster and it induces a current in the loop that sets up a magnetic field to oppose the magnet moving away i.e. the magnetic poles of the coil change.

p.d against time

Note: The p.d will be higher when leaving the coil as it will be moving quicker since it has been accelerated due to gravity.

This is because the magnet is moving faster as it exits and thus the rate of change in magnetic flux linkage is greater when it exits.

The p.d. changes direction because the current and the magnetic fields both switch to oppose the changes that occur.

## Faraday´s Law

Wire in Conductor

A length of wire, l, is part of a complete circuit cutting through a magnetic field of flux density, B

The conductor experiences a force of F= BIL. The force opposes the motion (Lenz’s law).

An equal and opposite force is needed for constant speed in the field

Work done can be calculated by force x distance, but force = BIL, so we can combine the equations to give (where ∆ means change)

We can also calculate the charge in the conductor

Since emf can be calculated by work done divided by charge, we get the following equations

Finally, since velocity = displacement / time

**This was Faraday’s Law**

Therefore, the induced emf in a circuit is equal to the rate of change of magnetic flux linkage through the circuit (Faraday). The direction of the induced current is always such that it opposes the change that causes the current (Lenz). The opposing change is represented by the negative sign in the equation:

**Example 1:** A conducting loop in the form of a circle placed perpendicular to a magnetic field of 0.80 T. if the radius of the loop increases from 10 cm to 20 cm in 1s, what is the induced emf in the loop?

** Solution:** We are given the following data: The magnitude of the magnetic field is B =0.8T. The initial radius of the loop is r1 = 10cm = 0.1m. The final radius of the loop is r2 = 20cm = 0.2m . The time is t = 1s. The expression for the induced emf in the loop is, ε = BA = B(πr2^2−πr1^2) t t Substituting the given values in the above expression, we will get ε = (0.8T)π((0.2m)^2−(0.1m)^2) 1s ε = 0.07539V ≈ 0.075V Thus,

**the induced emf in the loop is**0.075V

__Example 2__*Consider a solenoid of 9 turns with unknown radius, r. The solenoid is subjected to a magnetic field of 0.12 T. The axis of the solenoid is parallel to the magnetic field. When the field is uniformly switched to 12 T over a period of 2 minutes an emf with a magnitude of −0.3 V is induced. Determine the radius of the solenoid.*

__:__Start with Faraday’s Law ε = − NΔϕ Δt The area, A, is the surface area of the solenoid which is πr^2. *Solution:*

Interested in electrical and electronic engineering? Find out more about all the electrical engineering courses we have available by clicking __here__.

__Diploma in Electrical Technology__

__Diploma in ____Renewable ____Energy (Electrical)__

**Diploma in Electrical and Electronic Engineering**

Alternatively, you can view all our __online engineering courses here.__

## Recent Posts

### Understanding the mechanisms involved in a voltage amplifier

Understanding the mechanisms involved in a voltage amplifier In our previous articles, we discussed analogue signals and their characteristics. We’re going to dive a little deeper into analogue signals and see how a voltage amplifier works. What is an operational amplifier? Operational amplifiers, or op-amps, are one of the basic building blocks of analogue electrical […]

### Characteristics of analogue electronics

Characteristics of analogue electronics In our previous articles, we’ve discussed subjects such as the different types of semiconductors and how they work. We’re now going to focus on analogue electronics—what it is and its characteristics. What is an analogue signal? An analogue signal is continuous; in other words, it can have an infinite number of […]

### The structure and mechanism of a Bipolar transistor

The structure and mechanism of a Bipolar transistor In our previous article, we discussed the operation of metal oxide transistors, and now we’re going to have a look at bipolar transistors. We’ll look at their mechanism and how they work. What is a bipolar transistor? A bipolar junction transistor is a semiconductor device which can […]