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Abstract Measuring the value of a resistor with an ohmmeter is pretty simple. You connect the meter to the resistor, and read off the measurement from the meter. But what if the resistance you want to measure is very low? This project shows you how to use a four-point resistance measurement method to measure low resistance values.Objective The goal of this project is to determine which method for measuring small resistances (<1 kohm) is best: the two-point or four-point resistance measurement method? Introduction You probably have learned how to measure the resistance of a copper wire by using a multimeter. Ohmmeter measurements are normally made with just a two-point measurement method (one probe on each of the two resistor leads). However, when measuring very small resistances, in the milli- or micro-ohm range, the two-point method is not satisfactory because test contact resistance becomes a significant factor. A similar problem occurs when making ground mat resistance tests, because long lead lengths (up to 1000 feet) are used. Here also, the lead resistance, due to long lead length, will affect the measurement results. The four-point resistance measurement method eliminates lead resistance or contact resistance. In this project, we will show you a scientific way to accurately measure resistance by minimizing the contributon of contact resistance. The following description, from Tony Kuphaldt's website, AllAboutCircuits.com (Kuphaldt, 2003), explains:
"Suppose we wished to measure the resistance of some component located a significant distance away from our ohmmeter. Such a scenario would be problematic, because an ohmmeter measures all resistance in the circuit loop, which includes the resistance of the wires (Rwire) connecting the ohmmeter to the component being measured (Rsubject):
"Usually, wire resistance is very small (only a few ohms per hundreds of feet, depending primarily on the gauge (size) of the wire), but if the connecting wires are very long, and/or the component to be measured has a very low resistance anyway, the measurement error introduced by wire resistance will be substantial. "An ingenious method of measuring the subject resistance in a situation like this involves the use of both an ammeter and a voltmeter. We know from Ohm's Law that resistance is equal to voltage divided by current (R = V/I). Thus, we should be able to determine the resistance of the subject component if we measure the current going through it and the voltage dropped across it:
"Current is the same at all points in the circuit, because it is a series loop. Because we're only measuring voltage dropped across the subject resistance (and not the wires' resistances), though, the calculated resistance is indicative of the subject component's resistance (Rsubject) alone. "Our goal, though, was to measure this subject resistance from a distance, so our voltmeter must be located somewhere near the ammeter, connected across the subject resistance by another pair of wires containing resistance:
"At first it appears that we have lost any advantage of measuring resistance this way, because the voltmeter now has to measure voltage through a long pair of (resistive) wires, introducing stray resistance back into the measuring circuit again. However, upon closer inspection it is seen that nothing is lost at all, because the voltmeter's wires carry miniscule current. Thus, those long lengths of wire connecting the voltmeter across the subject resistance will drop insignificant amounts of voltage, resulting in a voltmeter indication that is very nearly the same as if it were connected directly across the subject resistance:
"Any voltage dropped across the main current-carrying wires will not be measured by the voltmeter, and so do[es] not factor into the resistance calculation at all. Measurement accuracy may be improved even further if the voltmeter's current is kept to a minimum, either by using a high-quality (low full-scale current) movement and/or a potentiometric (null-balance) system. "This method of measurement which avoids errors caused by wire resistance is called the Kelvin, or 4-wire method, or 4-point method. Special connecting clips called Kelvin clips are made to facilitate this kind of connection across a subject resistance:
"In regular, 'alligator' style clips, both halves of the jaw are electrically common to each other, usually joined at the hinge point. In Kelvin clips, the jaw halves are insulated from each other at the hinge point, only contacting at the tips where they clasp the wire or terminal of the subject being measured. Thus, current through the 'C' ('current') jaw halves does not go through the 'P' ('potential,' or voltage) jaw halves, and will not create any error-inducing voltage drop along their length: (Kuphaldt, 2003)"
Terms, Concepts, and Questions to Start Background Research To do this project, you should do research that enables you to understand the following terms and concepts:
Bibliography
Materials and Equipment To do this experiment you will need the following materials and equipment:
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| Note Before Beginning: This science fair project requires you to hook up one or more devices in an electrical circuit. Basic help can be found in the Electronics Primer. However, if you don't have experience in putting together electrical circuits you may find it helpful to have someone who can answer questions and help you troubleshoot if your project isn't working. A science teacher or parent may be a good resource. If you need to find another mentor, try asking a local electrician, electrical engineer, or person whose hobbies involve building things like model airplanes, trains, or cars. You may also need to work your way up to this project by starting with an electronics project that has a lower level of difficulty. |
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| Figure 1. Diagram for making 4-wire resistance measurements using two digital multimeters. |
Variations
Credits
Written by Charlie Zhai, 
Edited by Andrew Olson, Ph.D., Science Buddies
Sources
Last edit date: 2011-11-04 09:00:00
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