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Thermocouple electromotive force

Thermocouple electromotive force is affected by pressure. Usually the indicated temperature is slightly less than the true temperature. For example at 5.0 GPa and 1300°C, the Pt/PtlORh thermocouple indicates a temperature being about 50° C too low. The corrections are approximately linear with both pressure and temperature. [Pg.325]

TABLE 1.18. Tungsten and Tungsten-Rhenium Thermocouple Electromotive Forces at Various Temperatures for a Reference Junction at 0°C [1.39]... [Pg.37]

Thermocouples are primarily based on the Seebeck effect In an open circuit, consisting of two wires of different materials joined together at one end, an electromotive force (voltage) is generated between the free wire ends when subject to a temperature gradient. Because the voltage is dependent on the temperature difference between the wires (measurement) junction and the free (reference) ends, the system can be used for temperature measurement. Before modern electronic developments, a real reference temperature, for example, a water-ice bath, was used for the reference end of the thermocouple circuit. This is not necessary today, as the reference can be obtained electronically. Thermocouple material pairs, their temperature-electromotive forces, and tolerances are standardized. The standards are close to each other but not identical. The most common base-metal pairs are iron-constantan (type J), chomel-alumel (type K), and copper-constantan (type T). Noble-metal thermocouples (types S, R, and B) are made of platinum and rhodium in different mixing ratios. [Pg.1138]

ASTM E230-96el. Standard Specification for Temperature-Electromotive Force (EMF) Tables for Standardized Thermocouples. American Society for Testing and Materials, 1996. [Pg.1174]

Thermocouple An instrument for the measurement of temperature consisting of two wires of different metals joined at each end. An electrical electromotive force is generated, the magnitude of which allows the temperature to be measured. [Pg.1482]

As examples of properties of systems satisfying the conditions of definiteness at a particular temperature and of reversion, we may refer to the electrical resistance of a metal wire the electromotive force of a thermocouple with a fixed temperature at the cold junction the volume of a homogeneous gaseous, liquid, or... [Pg.2]

The Seebeck Effect The production of an electromotive force in a thermocouple under conditions of zero electric current. Thermoelectric power is the change in voltage at a thermocouple as a function of temperature. [Pg.428]

The working principle of the thermocouple was discovered (1823) by Seebeck who observed that if wires of two different metals were joined to form a continuous circuit, a current flowed in the circuit when the two junctions were at different temperatures. In order to make a measurement, one junction (the reference junction) is maintained at a constant temperature (typically at 0°C) and the electromotive force produced when the other junction is at the test temperature is measured, or recorded, by a suitable instrument (or used as the input of a controller ). In order to choose the right kind of thermocouple among the many types available, the temperature range to be studied must be considered, as well as several requirements regarding sensitivity, calibration stability, chemical, thermal, mechanical inertia, etc. [Pg.548]

A thermocouple manometer is a glass vessel with a tube for connection to a vacuum system. A heater is installed on two inlets to the vessel, while a thermocouple is welded to two other inlets. Its junction, in turn, is welded to the heater, to which a constant amount of heat is supplied. But since the heat conductivity of the residual gas in the system depends on the pressure, the withdrawal of heat from the heater is different at different pressures. Therefore, the temperature of the heater, which is measured by the thermocouple, also varies. The electromotive force (e.m.f.) produced will be proportional to the pressure. The millivoltmeter measuring the e.m.f. of the thermocouple is graduated in mmHg. Such a manometer can be used to measure a pressure from 10 to 10 mmHg. [Pg.44]

The most often used temperature detectors in renewable energy and most other processes are the thermocouples (TCs). Their operation is based on the principle known as the Seebeck effect. T. J. Seebeck discovered that heating the junction of dissimilar metals generates a small, continuous electromotive force (EMF). The name is a combination of thermo and couple denoting heat and two junctions, respectively. The dissimilar TC wires are joined at the hot (or measurement) end and also at the cold junction (reference end),... [Pg.510]

If the MWNT - PTFE composite material was deformed by rolling, and this deformed material combined with starting non-deformed composite, thermocouple was formed. Its thermo-electromotive force did not exceed 1 pV/K (Fig. 6). [Pg.761]

The use of the thermopile in the form of Le Chatelier Js 3 platinum, platinum-rhodium thermocouple, a so-called pyrometer, has obtained especial importance. This can be used to measure temperatures up to 17000.4 The electromotive force is measured either by one of the well-known methods, or else direct reading precision-voltmeters (or galvanometers), whose scales are divided both into millivolts and into the corresponding degrees Celsius or Fahrenheit, are employed. The determination of the... [Pg.239]

In a thermocouple, heating one junction of a bimetallic couple and cooling the other produces electromotive force in the circuit. This observation was originally was made by Seebeck in 1821. Besides the use of thermocouples, transistor electronics and semiconductors are important areas of interest for thermoelectric phenomena. Thermocouples made of semiconductors can develop relatively large electromotive potentials and are used to convert heat into electricity. [Pg.406]

Electrical methods. The electrical methods of measuring temperature are based on two facts, firstly, that the resistance of a conductor varies with the temperature, and secondly, that the electromotive force which is produced at a point of contact between two different metals or alloys is hkewise a function of the temperature. If, therefore, we close a circuit consisting of two wires of different metals, so that there are two joints in the circuit where two metals meet, a current will flow in general so long as these joints are not at the same temperature. If the temperature of the one joint is known, a measurement of the electromotive force enables us to determine the temperature of the other. On account of the great sensibility of electrical measurements, it is possible to measure very small differences of temperature by either of these methods. They have the further advantage over the first and second methods, that we are enabled by their means to measure very high and very low temperatures in a most convenient manner. The small bulk occupied by a thermocouple is often important from an experimental point of view, and for this reason thermocouples are preferable in some cases to all other forms of thermometer. [Pg.10]

We have the following relations between the temperature and the electromotive force of a thermocouple. The total e.m.f. is the difference between the e.m.f. s and eg at the hot and cold joints respectively. For a first approximation we may put... [Pg.12]

For metals of high melting point, Holborn and Day recommend the following procedure A wire of the metal about I cm. in length is placed at the junction of a thermocouple, and the electromotive force is measured as soon as the wire melts. In certain cases precautions must be taken to prevent chemical action with the atmospheric air. The table on page 44 gives the melting point h> and the latent heat of fusion w of the more important elements. [Pg.43]

This is the basic principle of thermoelectric pyrometry. The electromotive forces developed by thermocouples are small, usually a few thousandths of a volt. To measure such small electromotive forces special types of sensitive voltmeters (millivolt-meters) or indicators are required. For any particular type of couple these instruments may be graduated to read temperature directly instead of electromotive force. [Pg.419]

Metals Used for Thennocouples.— Although any two dissimilar metals might be employed for a thermocouple, certain combinations are unsatisfactory because of the very small electromotive forces which can be developed and because of the fact that with some combinations the electromotive force may... [Pg.419]

Reproducibility of Couples.—When thermocouples are employed in the laboratory for scientific purposes, although desirable, it is not of serious importance that the calibration or temperature-electromotive force relation of couples of the same type be exactly similar. However, in the industrial plant this question of reproducibility is of considerable moment. The indicating instruments are usually graduated in degrees of temperature and the graduation applies for one definite temperature-electromotive force relation only. If the temperature electromotive force relations of various couples of the same type are not similar, corrections must be applied to the readings of the indicator, and these corrections will be different for each couple. When several couples are operated with one indicator and when the process is such as to require a frequent renewal of couples, the applying of these corrections becomes very troublesome. [Pg.420]

Temperature of the Cold Jimctions of Thermocouples.—The electromotive force developed by a thermocouple depends upon the temperature of the cold... [Pg.430]

On the other hand, for slow reactions, adiabatic and isothermal calorimeters are used and in the case of very small heat effects, heat-flow micro-calorimeters are suitable. Heat effects of thermodynamic processes lower than 1J are advantageously measured by the micro-calorimeter proposed by Tian (1923) or its modifications. For temperature measurement of the calorimetric vessel and the cover, thermoelectric batteries of thermocouples are used. At exothermic processes, the electromotive force of one battery is proportional to the heat flow between the vessel and the cover. The second battery enables us to compensate the heat evolved in the calorimetric vessel using the Peltier s effect. The endothermic heat effect is compensated using Joule heat. Calvet and Prat (1955, 1958) then improved the Tian s calorimeter, introducing the differential method of measurement using two calorimetric cells, which enabled direct determination of the reaction heat. [Pg.236]

Tungsten-molybdenum thermocouples are useful, especially at high temperatures. They give an increase in electromotive force with an increase of temperature up to 540° C. and pass through zero millivolts at 1300° C. [Pg.275]

Thermoconples nnfortnnately develop only relatively small voltage (electromotive force, or emf) changes for a temperatnre difference of 1°C. Hence errors of predicted temperatures are often relatively large. The first three thermoconples often have errors of 2°C to 3°C or 0.5% to 0.75%. The latter three (and more expensive) thermocouples typically have smaller errors. With specially constructed thermocouples having purer metals, better connections, etc., errors are reduced by perhaps 50% as compared with the values reported above. [Pg.1532]


See other pages where Thermocouple electromotive force is mentioned: [Pg.402]    [Pg.9]    [Pg.402]    [Pg.240]    [Pg.419]    [Pg.420]    [Pg.420]    [Pg.421]    [Pg.422]    [Pg.426]    [Pg.427]    [Pg.427]    [Pg.428]    [Pg.429]    [Pg.457]    [Pg.457]    [Pg.457]    [Pg.466]    [Pg.468]    [Pg.1232]    [Pg.1233]    [Pg.36]    [Pg.9]    [Pg.687]   
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