Electric Motor

Fleming's Left Hand Rule

Fleming’s Left-Hand Rule is a simple tool that can be used to easily work out the direction of force acting on a current-carrying wire in a magnetic field. Using your left hand, hold your thumb, index finger, and middle finger at right angles to each other, as shown above. Then, point your index finger in the direction of the magnetic field (north to south) and your middle finger in the direction of the current (+ to -). Your thumb then points in the direction of the resulting force on the wire!

Types of Electric Motors

There are countless different variations of an electric motor design for various applications, but they fall into two main classifications: Alternating current (AC) motors and direct current (DC) motors.

DC Motors

The simplest form of DC motor consists of a stationary magnetic field and a conductor coil connected to a split ring commutator, which is connected to a DC power supply via brushes. The diagram below shows this type of motor in a starting position.

Diagram showing components of a very simple DC motor, and how these create a rotational force around the motor axis. Ross MacDonald, StudySmarter Originals.

Now, let's take a look at how a DC motor works step by step:

1. As a voltage is applied to the brushes, the split ring commutator passes this voltage to the coil which creates a current on the coil. The current-carrying coil is in a magnetic field, so the motor effect produces an opposite force on each side of the coil as the current is travelling in opposite directions. This creates a rotational force on the coil, and in this example the motor begins to rotate anticlockwise.

2. After rotating by 90 degrees from the starting position, the split ring commutator reverses the direction of the current. This causes the side of the coil at the top of the rotation to now experience a force downwards, and the side of the coil at the bottom of the motor to experience a force upwards. Combined with the momentum from the initial rotation, this continues to accelerate the coil in an anticlockwise rotation.

3. After rotating a further 180°, the split ring commutator again reverses the current direction and changes the direction of the forces on the coil. This accelerates the coil through the next half-turn, and this sequence continues as the motor spins.

To increase the power of a DC motor, there are three main approaches:

• Increasing the strength of the magnetic field. This increases the$\mathit{B}$term in the motor effect equation, creating a stronger force on the coil.

• Adding more turns (loops) to the coil. This increases the total length of the coil, increasing the$\mathit{L}$term in the motor effect equation and producing a stronger force.

• Using a higher current in the coil. This increases the$\mathit{I}$term in the motor effect equation, creating a stronger force.

The performance can also be improved by adding an iron core to the electromagnet rotor, as is shown in the more typical DC motor below.

Diagram of a typical DC motor, showing the rotor coil with many loops and an iron core to improve performance. Wikipedia.

A more advanced type of DC motor is the brushless motor. As the name suggests, the main difference in this type of motor is that it does not have the split-ring commutator or brush components. Instead, the DC supply voltage polarity is digitally varied using a semiconductor controller. This has the advantage of improved reliability, since the brushes often wear out in brushed motors and need to be replaced, and provides a better performance overall.

AC Motors

AC motors work using a similar principle to DC motors, but with several key differences. Generally, the coil windings form the stator (stationary part) of the motor, while the rotor is a permanent magnet or electromagnet.

In an AC power supply the voltage varies sinusoidally from positive to negative, as shown below. When an AC voltage is applied to the electromagnet stator coil windings, the varying voltage produces a varying magnetic field. In an AC motor, this varying magnetic field is used to produce a rotational force on the rotor and spin the motor. The split-ring commutator is no longer needed, since the current direction is reversed by the AC supply.

(Top) - Sinusoidal variation of voltage in an AC power supply. (Bottom) - Corresponding magnetic field strength & direction produced by an electromagnet with an AC voltage applied. Ross MacDonald, StudySmarter Originals

Electric Motor Functions

Electric motors are found in countless devices we interact with every day. Household devices will generally use a DC motor if they are battery powered, and an AC motor if they are mains powered. This is to avoid having the convert the power supply from AC to DC or vice-versa, which would decrease efficiency and increase cost due to the extra components required. Below, you can see the applications of DC and AC motors in everyday use.

Household DC Motors:

• Electric toothbrush
• Laptop cooling fan
• Remote-controlled car
• Battery-powered drill
• Vibration motor in a game controller
• Car starter motor

Household AC Motors:

• Extractor fan
• Kitchen electric mixer
• Vacuum cleaner
• Washing machine
• Microwave

Electric Motor Power Calculation

When calculating the power of an electric motor, there are two variables you should consider, the output power and the input power.

The output power of an electric motor

As power is equal to energy-per-second, we can calculate the output mechanical power of a motor by measuring the time taken to perform a known amount of work. A simple experiment design to do this could use a motor to lift a mass by winding it up on a string.

We know that work done is equal to a force multiplied by the distance its applied over:

$\mathrm{work}\mathrm{done}\left[\mathrm{J}\right]=\mathrm{force}\left[\mathrm{N}\right]\times \mathrm{distance}\left[\mathrm{m}\right]$

The mechanical power of the motor (which is the output power of a motor) is found by dividing the amount of useful work done by the number of seconds it took to complete the work.

$P_{Mech}\left[\mathrm{W}\right]=P_{Out}\left[W\right]=\frac{\mathrm{work}\mathrm{done}\left[\mathrm{J}\right]}{\mathrm{time}\mathrm{taken}\left[\mathrm{s}\right]}$

Input Power of an electric motor

The electric motor input power can be found using the general electric power equation. Note that this can be done because the input power of an electric motor is electrical power.

$P_{Elec}=P_{In}=\mathrm{Voltage}\left[\mathrm{V}\right]\times \mathrm{Current}\left[\mathrm{A}\right]$

Electric Motor Efficiency

The efficiency of a device is a way of measuring how much of the energy you put in is converted into useful output energy. A general formula for the efficiency of a device is:

$\mathrm{Efficiency}=\frac{\mathrm{useful}\mathrm{output}\mathrm{power}}{\mathrm{input}\mathrm{power}}$

For an electric motor, the input power is electrical and the output power is mechanical. The main source of waste energy in an electric motor is heat – this is produced both by the electrical resistance of the wire coils and friction between moving and static components.

The motor efficiency can be calculated by dividing the useful mechanical power output by the total electric power input. This is converted to a percentage efficiency by multiplying by 100.

${\mathrm{Efficiency}}_{motor}=\frac{P_{mechout}}{P_{elecin}}\times 100\%$