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Ammeter and Voltmeter An ammeter is used to measure the current through a resistor R that forms part of a circuit. It must be connected in series to the resistor so the current will go through it. In order not to disturb the rest of the circuit, the combination of the resistor and the ammeter must have an equivalent resistance similar to the original resistance R . If RA is the resistance of the ammeter, the condition Req = R + RA » R requires that the ammeter has very small resistance. A voltmeter is used to measure the voltage across, or the potential difference between the two leads of, a resistor. Again in order not to disturb the rest of the circuit, the combination of the resistor and the voltmeter must have an equivalent resistance similar to the original resistance. If RV is the resistance of the voltmeter, the condition 1 1 1 1 = + » Req R RV R requires that the voltmeter has very large resistance. At the heart of the ammeter or voltmeter is a galvanometer. For our purpose, it is just a device that senses the current when connected into a circuit. It has resistance RG . The maximum current that goes through it without damaging it is denoted by IG,max , and is related to the maximum voltage VG,max across it by Ohm’s law: VG,max = IG,max RG In an ammeter, a resistor called the shunt resistor RS is connected in parallel with a galvanometer in order to reduce the overall resistance. The ammeter resistance is therefore given by 1 1 1 = + RA RG RS The requirement of small resistance is satisfied if RS is very small, so that RA » RS . When an ammeter is used to measure the maximum current I max it can handle, the galvanometer current reaches the value IG,max . Referring to the diagram below, where it is seen that the galvanometer and the shunt resistor share the same voltage difference, we have ( Imax - IG,max ) RS = IG,max RG = VG,max Because RS << RG , we have I max >> IG,max . It follows that I max = VG,max RS Thus different scales for the ammeter can be chosen by using different shunt resistances. In a voltmeter, the shunt resistor is connected in series with the galvanometer. Therefore RV = RG + RS » RS The last approximation is because a voltmeter should have very large resistance so that RS >> RG . When it is used to measure the maximum voltage Vmax it can handle, the same current IG,max goes through the galvanometer and the shunt resistor, while the voltages across them are VG,max and Vmax -VG,max respectively. From Ohm’s law: Vmax -VG,max VG,max = = IG,max RS RG Since RS >> RG implies Vmax >> VG,max , it follows that Vmax = IG,max RS Again different scales for the voltmeter can be chosen by using different shunt resistances.