# Velocity of free electrons in a wire

The free electrons in a metal have three distinct velocities associated with them:
(a) a random velocity ( about 105 ms-1)
(b) a velocity with which electrical energy is transferred along the wire (about 108ms-1)
(c) a drift velocity of the electrons as a whole when a current flows through the wire (this depends on the applied voltage but is usually a few mms-1 for currents of a few amps in normal connecting leads).

The diagram in Figure 1 shows a simplified and enlarged view of a section of a wire carrying a current. The electrons are in random motion but if a potential difference is applied across the wire with the right hand end positive the free electrons drift slowly towards that end.

### schoolphysics: Electric current animation

To see an animation of the movement of free electrons in an electric current click on the animation link.

It is possible to measure the electron drift velocity (v) using the experiment outlined in the following Student Investigation.

Student Investigation

It is not possible to measure the electron drift velocity in a metal directly but an idea of its value can be found by measuring the drift velocity of ions in a liquid.

A piece of filter paper should be clipped to a microscope slide and then soaked with a dilute solution of ammonium hydroxide. A crystal of potassium permanganate should be put on the paper and a voltage applied between the two clips. The coloured manganate ions can be seen to move and their velocity can be measured. (Figure 2).

Record the variation of drift velocity for voltages between 50V and 200V.

DANGER:
Take care not to touch the H.T terminals during the experiment.
Current output must be limited to 5 mA

Student investigation

Devise and carry out an experient to investigate the conduction of electricity along different pencil lines drawn on a piece of paper.

### Electron drift velocity

You can work out an equation for the electron drift velocity as follows:

Consider a wire of cross sectional area A and carrying a current I amps. Let the number of free electrons per unit volume be n and the drift velocity be v. (See Figure 3).

In one second an electron will have moved a distance v down the wire but since there are n electrons per unit volume the total number moving through this distance will be nAv. Therefore since the charge on an electron is e the current I (which is the charge moving past any point in the wire) is:

Current (I) = nAve

The table below shows some free electron concentrations

 Metal Free electron concentration (m-3) (at 300 K) Lithium 4.7x1028 Sodium 2.7x1028 Silver 5.9x1028 Copper 8.5x1028

Example problems
1. Calculate the drift velocity of electrons in a copper wire of cross sectional area 2x10-7 m2 (0.5mm diameter) carrying a current of 0.5A. (n = 8.5x1028)
v = I/nAe = 0.5 /[8.5x1028x2x10-7x1.6x10-19] = 1.84x10-4ms-1 = 0.184mms-1

2. A motorist switches on their headlights. If the distance along the copper connecting wires between the car battery and one of the lights is 1.5 m what is the average time that an individual electron will take to drift between the battery and the light? Take the current in the wire to be 3A, and the cross sectional area of the wire to be 3x10-7 m2.
v = I/nAe = 3 /[8.5x1028x3x10-7x1.6x10-19] = 7.4x10-4ms-1 = 0.74 mms-1
Therefore time taken = 1.5/7.4x10-4 = 4080 s = 1.13 hours

### The electron steeplechase

When a current flows round a series circuit the current at any point in the circuit is the same. The same number of electrons flow past any point in the circuit every second - no electrons are lost. Although the number of electrons is always the same their energy gets less as they move round the circuit.

This energy appears as heat, light or magnetism in say an electrical heater, a light bulb or an electromagnet.

You can compare this energy loss with the change in energy of runners in a steeplechase. The energy loss of the athletes when going over the barriers represents the energy that electrons transfer when they pass through a resistor.

A VERSION IN WORD IS AVAILABLE ON THE SCHOOLPHYSICS USB

© Keith Gibbs 2020