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The original meaning of the term potentiometer, which is still in use, is an apparatus used to measure the potential (or voltage) in a circuit by tapping off a portion of a known voltage from a resistive slide wire and comparing it with the unknown voltage by means of a voltmeter or galvanometer. The present popular usage of the term potentiometer (or 'pot' for short) describes an electronic component which has a user-adjustable resistance. Usually, this is a three-terminal resistor with a sliding contact in the center. If all three terminals are used, it can act as a variable voltage divider. Potentiometer as measuring instrument
Constant current potentiometer This is used for measuring voltages below 1.5 volts. In this circuit, the unknown voltage is connected across a section of resistance wire the ends of which are connected to a standard electrochemical cell that provides a constant current through the wire, The unknown emf, in series with a galvanometer, is then connected across a variable-length section of the resistance wire using a sliding contact(s). The sliding contact is moved until no current flows into or out of the standard cell, as indicated by a galvanometer in series with the unknown emf. The voltage across the selected section of wire is then equal to the unknown voltage. All that remains is to calculate the unknown voltage from the current and the fraction of the length of the resistance wire that was connected to the unknown emf. The galvanometer does not need to be calibrated, as its only function is to read zero. When the galvanometer reads zero, no current is drawn from the unknown electromotive force and so the reading is independent of the source's internal resistance Constant resistance potentiometer The constant resistance potentiometer is a variation of the basic idea in which a variable current is fed through a fixed resistor. These are used primarily for measurements in the millivolt and microvolt range. Microvolt potentiometer This is a form of the constant resistance potentiometer described above but designed to minimise the effects of contact resistance and thermal emf. This equipment is satisfactorily used down to readings of 10 nV or so. Thermocouple potentiometer Another development of the standard types was the 'thermocouple potentiometer' especially modified for performing temperature measurements with thermocouples. * Potentiometer as electronic component
Low-power types
Linear potentiometers A linear pot has a resistive element of constant cross-section, resulting in a device where the resistance between the wiper and one end terminal is proportional to the distance between them. Linear describes the electrical 'law' of the device, not the geometry of the resistive element. No Logarithmic potentiometers A log pot has a resistive element that either 'tapers' in from one end to the other, or is made from a material whose resistivity varies from one end to the other. This results in a device where output voltage is a logarithmic (or inverse logarithmic depending on type) function of the mechanical angle of the pot. Most (cheaper) "log" pots are actually not logarithmic, but use two regions of different, but constant, resistivity to approximate a logarithmic law. A log pot can also be simulated with a linear pot and an external resistor. True log pots are significantly more expensive. High-power types
Digital control See digitally controlled potentiometer. Transducers Potentiometers are also very widely used as a part of displacement transducers because of the simplicity of construction and because they can give a large output signal. Audio control
Theory of operation The 'modern' potentiometer can be used as a potential divider (or voltage divider) to obtain a manually adjustable output voltage at the slider (wiper) from a fixed input voltage applied across the two ends of the pot. This is the most common use of pots. The voltage across is determined by the formula: V_mathrm = cdot V_s The parallel lines indicate components in parallel. Expanded fully, the equation becomes: V_mathrm = cdot V_s Although it is not always the case, if is large compared to the other resistances (like the input to an operational amplifier), the output voltage can be approximated by the simpler equation: V_mathrm = cdot V_s As an example, assume V_mathrm = 10 mathrm, , , and . Since the load resistance is large compared to the other resistances, the output voltage will be approximately: cdot 10 mathrm = cdot 10 mathrm approx 6.667 mathrm Due to the load resistance, however, it will actually be slightly lower: ≈ 6.623 V. One of the advantages of the potential divider compared to a variable resistor in series with the source is that, while variable resistors have a maximum resistance where some current will always flow, dividers are able to vary the output voltage from maximum () to ground (zero volts) as the wiper moves from one end of the pot to the other. There is, however, always a small amount of contact resistance. In addition, the load resistance is often not known and therefore simply placing a variable resistor in series with the load could have a negligible effect or an excessive effect, depending on the load. Early patents See also Linear taper | |||||||||||||||||
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