Electricity Tutorial 1 - Basic Electrical Measurement

 Contents

Measuring Instruments

The instruments that are of most use to the physicist and the electrical engineer are the voltmeter and ammeter.  With these, we can directly measure:

• Potential Difference (or voltage)

• Current.

We can then use the data to get:

• Resistance (volts ÷ amps);

• Power (volts × amps).

The multimeter is often used, as it can measure voltage and current (but not at the same time).

Notice that there is an analogue meter (a meter with a scale) and a digital meter (a meter where the read-out is a number).  It is important that you learn how to use these instruments correctly in your practical work.  If in doubt, ask your teacher.

Current is measured with an ammeter, which is wired in series with the component.  The voltmeter is wired in parallel with the component.

Circuit Diagrams

The diagram above is a circuit diagram.  It shows how the components are connected together.  It uses standard symbols which all electrical engineers will understand.  You do not have to be an artist to draw one, but follow these simple rules:

• Use a pencil and a ruler;

• Draw the lines horizontally and vertically;

• Ensure that all the components are there, including the power supply;

• Use the correct symbols;

• Where there are junctions (wires joined together), there is a black circle, which represents a blob of solder.

You knew that anyway, didn't you?

There is a document that shows all the commonly used symbols.  It is a .pdf file and you can access it HERE.

In word-processed documents, use graphics to produce a circuit diagram if you can.

## Current and Charge

The base electrical quantity is current, the flow of charge.  All other electrical quantities are derived from it.  Current is measured in ampères, or amps (A).

Charge is measured in coulombs (C), which is defined as:

1 coulomb is the quantity of charge carried past a given point if a steady current of 1 amp flows for 1 second.

1 C = 1 A s-1

A single electron carries a charge of 1.6 × 10-19 C.

1 coulomb is equivalent to 6.2 ´1018 electrons.  It is much more convenient to use this rather than counting individual electrons.  You would buy a 1 kg bag of sugar rather than counting all the crystals in it.

All charges have a whole number multiples of the electronic charge, e.  We say that charge is quantised.

 What do you think an electron is?

Charge and current are linked by a simple formula:

Charge (C) = current (A) ´ time (s)

Q = It

In the syllabus the formula is written in physics code as:

The symbol D is Delta, a Greek capital letter 'D', meaning “change in”.

There are some important multipliers for current:

• 1 microamp (1 mA) = 1 ´ 10-6

• 1 milliamp (mA) = 1 ´ 10-3 A

These are useful when we are dealing with small currents.  However we must remember to convert to SI units for doing calculations.  Watch out for this bear trap!

 Show that 1 coulomb is 6.2 ´1018 electrons. A charge of 1.24 C flows in a period of 0.63 s.  What is the current?

Potential Difference

Potential Difference is defined as energy per unit charge transferred to useful energy by the circuit. Electromotive force (E.m.f.) is the energy per unit charge supplied by the source to the circuit.  We will look at this in more detail in Electricity Tutorial 8.

The unit of potential difference is the volt (V).  Using the definition, we can define the volt as Joules per Coulomb

1 V = 1 JC-1.

Potential difference (V) = energy converted (J)

Charge (C)

In physics code we write:

Potential difference is often referred to as voltage.

Conventional current goes from positive to negativeElectrons carry energy around the circuit; they go from negative to positive.  In the early days, physicists didn't know about the electron, which is why they got it all wrong.  Correction would require a complex re-write of the Laws of Physics, a task which no-one is likely to be bothered to tackle.  So all conventional currents are from positive to negative.  All currents are treated as conventional.

Sources of Voltage

Examples of sources of voltage include:

• Car batteries;

• Dry cells;

• Rechargeable cells;

• Mains;

• Generators.

#### This is because the voltage of the parallel combination is 1.5 V

The two cells in the parallel combination will last twice as long, since the current will be half that taken from the two series cells.

Batteries are often rated in amp-hours.  A 1 amp hour battery can give out a current of 1 amp for 1 hour.  The charge contained is:

Q = 1 A × 3600 s = 3600 C

 A cordless drill operates using a 14.4 V battery pack.  The battery is rated at 2 amp hours which means that it can deliver a current of two amps for a period of 1 hour.  How much energy is held by the battery?

Resistance in a wire is the opposition of a wire to the flow of electricity.  It is caused by collisions between the electrons and the atoms in the wire.  The hotter the wire, the more chance there is of a collision.  Therefore hot wires have more resistance.  The formula for resistance is:

Resistance (ohms) = potential difference (volts)

current (amps)

In physics code we write this as R = V/I

Or more commonly:

V = IR

The unit for resistance is ohm (W).  (The curious symbol ‘W’ is Omega, a Greek capital letter long Ō.)

An alternative unit for ohms is volts per ampère:

1 W = 1 V A-1

What do you understand by the term resistance?

Use the circuit below to answer the questions:

##### R

(a)

0.30 A

18 W

(b)

12 V

88 W

(c)

14.4 V

0.52 A

 Watch out for these bear traps in electrical calculations:   Time must be in seconds   Make sure you convert milliamps to amps

Measuring Electrical Quantities
We can measure voltage and current using a circuit like this. You will be familiar with this from GCSE, and you will be expected to set it up as a matter of course.

The voltmeter is wired in parallel with the component, and the ammeter is wired in series with the components.

Normally we treat the instruments as perfect.  This means that:

• An ammeter has zero resistance.

• A voltmeter has infinite resistance.

In reality an ammeter has a very low, but measurable resistance.  Normally we ignore this.

Analogue voltmeters have a high resistance.  Normally this has little effect, but if we are measuring high value resistances, the current taken by the voltmeter can alter the result.

A digital voltmeter has a very high resistance indeed, and can be regarded as perfect.

A voltmeter can be calibrated to give a reading that is not a voltage.  For example an electronic thermometer gives out a variable voltage, but this is shown as a temperature.  The picture below shows a voltmeter calibrated as a photographer's light meter.

Image by El Grafo, Wikimedia Commons

At a certain light level, the electronic circuitry gives out a particular voltage.  The photographer doesn't need to know what that voltage is.  Instead she needs to interpret the output into the shutter exposure and the aperture of the lens.  The calibration is done by the manufacturer.

A more modern device has a digital output:

The output is a direct readout, so no skills interpreting the meter are needed.

Meters of known resistance (A-level)

This kind of problem is likely to appear in A-level papers rather than AS-level.

An analogue meter can be made to measure voltage or current by adding an external resistor:

• An ammeter uses a shunt, which is a low value resistor connected in parallel;

• A voltmeter uses a multiplier, which is a high value resistor connected in series.

You can't have the two on at the same time!  A typical meter found in a school laboratory is shown below:

Notice that there are separate shunts for AC and DC.  There is also a separate multiplier for AC voltage.

The picture shows the shunt resistors and the multiplier resistors in an analogue multimeter:

The same applies to digital multimeters, but the shunts and multipliers are not so easy to identify.

The real voltmeter has a circuit diagram like this:

A perfect voltmeter has an infinite resistance.  A digital voltmeter has a very high resistance, and can be considered to be almost perfect.  An analogue voltmeter will have a resistance of about 50 kilohms.  We model the voltmeter of known resistance as a perfect voltmeter in parallel with a known resistance:

 The circuit diagram shows how the meter is MODELLED.    The multiplier is actually wired in series.

 Worked example A voltmeter of resistance 35 kW is used to measure the voltage across a 350 kW resistor.  The source providing the current can be modelled as a voltage source of 2.0 V with an internal resistance of 45 kW.  (a) What is the voltage across the 350 kW resistor when the voltmeter is NOT connected?  (b) What is the voltage that is actually read from the meter? Answer We model the circuit like this: (a) We need to find the total resistance of the circuit: R = 45 000 W + 350 000 W = 395 000 W  Work out the current: I = 2.0 V ÷ 395 000 W = 5.06 × 10-6 A  Now work out the voltage across the 350 kW resistor: V = 5.06 × 10-6 A × 350 000 W = 1.77 V = 1.8 V (2 s.f.)   (b)  A voltmeter with a known resistance is treated as a perfect voltmeter in parallel with a known resistor.  With the voltmeter added our circuit becomes:    Now we need to work out the parallel combination of resistors: R-1 = (350 000 W)-1 + (35 000 W)-1 = 31.4 × 10-6 W-1 R = 31818 W   Now our circuit with the perfect voltmeter becomes: Now we work out the total resistance: R = 45 000 W + 31818 W = 76818 W   Then we can work out the current: I = 2.0 V ÷ 76818 W = 26.04 × 10-6 A   Finally we work out the voltage read by the meter: V = 26.04 × 10-6 A ×  31818 W = 0.828 V = 0.83 V (2 s.f.)   Note that the rounding appropriate significant figures is done at the last step.

A perfect ammeter has zero resistance.  While we can get a very nearly perfect voltmeter with a digital instrument, the same does not apply to an ammeter.  There is always a small resistance to the ammeter.  A real ammeter is a meter in parallel with a low value resistor called a shunt.  You will sometimes find in engineering text-books references to motors being shunt-wound.  This simply means that the rotor coils and the field coils are wired in parallel.

The meter is reading the voltage across the shunt resistance.

We model the ammeter as a perfect ammeter (i.e. one with zero resistance) in series with a resistor of known resistance, like this:

 (Challenge - Revise internal resistances of cells before trying this one out) The circuit shows a battery of EMF 20.0 V that has an internal resistance of 0.45 W.  It is connected to a 350 W resistor.  The potential difference is measured using a voltmeter of resistance 35 kW, while the current is measured using an ammeter of resistance 0.50 W.  The circuit is shown in the diagram below:     (a) Show that the current from the cell is about 58 mA. (b) Calculate the reading of the voltmeter, which is known to be accurately calibrated.

Using these values, there is not a great deal of difference compared to using ideal meters.  However with very high value resistors, as shown in the worked example, the differences become more obvious.

A multimeter can also be used as an ohmmeter.  In this case, the meter has a battery, and it measures the current.  The scale has its zero point when the maximum current is shown.  When zero current flows, the resistance is infinity.

The limitation is for high resistances.  Try measuring 7600 ohms with this scale.