




Syllabus Sections: 10a Meters 10a.1 Understand the use of multiplier resistors in analogue voltmeters, shunts in ammeters and the effect of the test meter on the circuit under test. Meters Analogue and Digital Despite the popularity of digital voltmeters (DVMs) meters with a numbers display, there is still a requirement for analogue meters with a moving needle display, especially in the Amateur Radio field, where we are often watching voltages/currents which are changing value, and, we may be looking, or "tuning" for, a maximum or minimum value.
The above operations are very difficult using a DVM as the voltage/current value is sampled at intervals with a hold delay between samples where as the analogue meter the needle swings up to the valve. The analogue meter is used if you wish to detect a slow change in values which is not possible with the digital meter. Notice the dials on the front of each meter these are used to select the range of the display. For the analogue meter this is particularly important so that the meter needle is not driven hard against the end stop due to the measured voltage being higher than the range. Multiplier Resistors for voltages and Shunts for Current in Analogue meters The dial on the meter is a multi position switch used to select from a range of voltages or current. These ranges are calibrated for correct full scale deflection (F.S.D.) by using multiplier resistors for measuring voltages and shunt resistors for measuring currents. The values of these resistances are determined by :
Measuring Voltage on an Analogue meter Note: Voltage are measured using the meter in parallel with the circuit under consideration. A 10V FSD VOLT METER Let's look at a typical example of an analogue multimeter. If we have a basic meter movement which has I FSD = 1 milliamp and R coil = 100 ohms. So what voltage applied to the meter gives the FSD. From V = I x R V = 0.001 x 100 = 0.1 volts. Use of multiplier resistor Such a low voltage would not be measured very often !! So what can we do to make the meter read 10V FSD on say switch position 1  use a series resistor which is called a "Multiplier". If we apply 10V to the meter without a multiplier resistor it would cause the needle to swing hard over and possibly break the meter. We know that 10V DC must cause a current of 1mA to flow through the meter for FSD, so we need to calculate what resistance will cause a current of 1mA to flow when 10v is applied. Using ohm's law V = I x R rearranged R = V / I = 10 / 0.001 = 10000 ohms or 10k
BUT we have not considered the coil's resistance = 100R, and this would cause errors in reading. If we used the 10k we would have a total series resistance is 10,100R and therefore the calculation which gives I = V / R = 10 / 10,100 = 0.99mA through the meter and do not achieve the 1mA FSD  there is a 1% error. The solution is to subtract 100 ohms from 10k  thus 10,000  100 = 9900 ohms. This 9900 ohms resistor is the "Multiplier". 100V FSD VOLT METER Similarly, if we require a FSD of 100V we must use a series resistance of : R = V_{(FSD)} / I_{(coil)} less 100 ohms thus ( 100 / 0.001 )  100 = 99,900 ohms Two points to note are :
Our Multimeter so far
Note that the meter need two scales 0 to 10 and 0 to 100 if you want direct reading. Measuring Current 1 amp range Note: Current passing is measured using the meter in series with the circuit under consideration. Let's say we want to measure a DC current of 1 amp flowing from a 12V battery to a 12 watt lamp. We are using the same meter as before so there must still be only 1mA through the meter ANY MORE and we "blow" the movement!!! Shunt resistor Thus we must divert 999 milliamps past the meter movement! This time we use a "SHUNT" resistor across the meter movement  in parallel with the meter  BUT of what value ??
What is the voltage between points A and B through the meter coil? 1mA in 100 R, gives V_{AB}= I x R = 0.001 x 100 = 0.1 volts Now in R_{shunt} I = 999mA and the V = 0.1 volts ( the voltage is the same as the resistors are in PARALLEL ). therefore R_{shunt} = V / I = 0.1 / 0.999 = 0.1001R NOTE: The higher the current range, the smaller R_{shunt} becomes. These resistors, which carry HIGH CURRENTS, are normally made from resistance wire such as "Constantan wire", or even copper bus bar ( a thick piece of copper ) for very high currents. If you unsure about current value, always start with highest range and switch down the ranges as required. Meter sensitivity The quality of a multimeter is usually quoted in "ohms per volt". If we look at our example above, on the ten volt range we have input resistance of 10k, which we can say is 10k ohms per 10V which equals 1000 ohms per volt. Similarly, on the 100v range, the input resistance is 100k. 100k for 100v gives the same 1000 ohms per volt. Our meter sensitivity is 1000 ohms per volt, pretty poor, when a good "AVO" is 20,000 ohms per volt. Our Voltage and Current Multimeter so far Let's build up our multimeter. So far, we will need a pair multi position switches (which have a current limit of about 5 amps at low voltages), or a rotary wafer switch, (which are expensive but have a higher current carrying capability) with the following positions:
The OFF position is used to place a short across the meter movement. This tends to stop the moving coil movement when subjected to shock if it were dropped (similar to how a short across motor feed has a breaking effect on the armature) A further position on the switch would be useful to provide a 5 or 10 amp range according to the switch(s) used. This additional position is included in the drawing below. We will leave it to you to calculate the value of the shunt resistor R_{x}
Here is the last part of the syllabus mentioned above and the effect of the test meter on the circuit under test. Looking at "our" multi, and we will attempt to use it to measure DC voltages in a typical circuit. As the HT+ve is 9V in our test circuit we can use the 10V range on our meter and we know that the resistance between the meter leads is 10K ohms ( if you are not certain about this look at the top of the page and then come back to here).
The 10k of the meter will load the circuit, "How ?" You might ask. Like this 
Thus total current passing, from Ohm's Law and as there are two resistors we will call that I_{TOTAL} so I_{TOTAL}= 9 / 59090 = 0.0001523 A say 0.00015 A Thus voltage drop through the 50k resistor is V = 0.00015A x 50000 = 7.5V Therefore Voltage at point V is 1.5V. So we are reading 1.385 volts at a point, normally at +6V !! A better meter would give a near correct reading but there will still be an error, which we should be able to estimate and make a decision that the reading of "OK", if we understand the test meter's limitations. the effect of the test meter on the circuit under test Meters can load a circuit and give an apparent error in the reading! BUTWe must also be aware that even a "digital" voltmeter and oscilloscopes, etc, present a resistance (or impedance!) to circuits under test. The average oscilloscope probe has an input resistance of 1 Megohms. Where it is used to examine HIGH IMPEDANCE circuits (oscillators for example) the probe may have a 10:1 multiplier, raising the I/P resistance to 10 Megohms and reducing the input capacitance. There two types of this probe: PASSIVE. This contains a resistor network which increases the input resistance x 10 and a resultant voltage reduction of 10 ACTIVE. This includes an amplifier circuit which multiplies the input resistance by say 10 without reducing the input voltage.
Of interest but the following is not in the syllabus RESISTANCE MEASUREMENT Whilst not part of the syllabus let's, briefly and ignoring the coil resistance, look at circuit A below.
With the meter terminals shorted as shown the current will be 1mA, giving us a FSD (Full Scale Deflection, which indicates zero ohms and the scale would be marked as such. If we now connect a 1k5 resistor across the terminals, as shown in circuit B below.
The total resistance is now 3k which is passing a current of 1/2mA which gives a half scale deflection and would be marked on the scale 1500 ohms. By the use of other resistors you would be able to mark up the scale. You would find that the scale is nonlinear and will be very cramped at the high resistance end of the scale. Our Voltage, Current and Resistance Multimeter
The meter is based upon the single pole 12 way switches which have limited current carrying capabilities  but as this is for demonstration purposes only high current will not be measured.
Valve Voltmeter VVM Valve Voltmeters are analogue meters, generally using a meter such as we have been describing in our multimeter above. The difference is that in the VVM there is a current amplifying circuit between the probe and the meter, giving an input resistance in the megohms range, with, therefore, very little loading on the circuit being measured. The amplifier was originally a valve type but may now be a transistor or operational amplifier used. For work on very high resistance circuits a bridge circuit is employed which, when balanced, draws no current from the circuit under test. These units are often called Voltage Measurement Units (VMUs) with very accurate measurements to +/ 0.1% or better.
NB R_{x} for the 5 amp range = 0.020004 R




