Pyrometer

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An optical pyrometer Gluehfadenpyrometer.jpg
An optical pyrometer
A sailor checking the temperature of a ventilation system. Pyrometer 040824.jpg
A sailor checking the temperature of a ventilation system.

A pyrometer or radiation thermometer is a type of remote sensing thermometer used to measure the temperature of distant objects. Various forms of pyrometers have historically existed. In the modern usage, it is a device that from a distance determines the temperature of a surface from the amount of the thermal radiation it emits, a process known as pyrometry, a type of radiometry .

Contents

The word pyrometer comes from the Greek word for fire, "πῦρ" (pyr), and meter, meaning to measure. The word pyrometer was originally coined to denote a device capable of measuring the temperature of an object by its incandescence, visible light emitted by a body which is at least red-hot. [1] Infrared thermometers, can also measure the temperature of cooler objects, down to room temperature, by detecting their infrared radiation flux. Modern pyrometers are available for a wide range of wavelengths and are generally called radiation thermometers. [2]


Principle

It is based on the principle that the intensity of light received by the observer depends upon the distance of the observer from the source and the temperature of the distant source. A modern pyrometer has an optical system and a detector. The optical system focuses the thermal radiation onto the detector. The output signal of the detector (temperature T) is related to the thermal radiation or irradiance of the target object through the Stefan–Boltzmann law, the constant of proportionality σ, called the Stefan–Boltzmann constant and the emissivity ε of the object.

This output is used to infer the object's temperature from a distance, with no need for the pyrometer to be in thermal contact with the object; most other thermometers (e.g. thermocouples and resistance temperature detectors (RTDs)) are placed in thermal contact with the object, and allowed to reach thermal equilibrium.

Pyrometry of gases presents difficulties. These are most commonly overcome by using thin filament pyrometry or soot pyrometry. Both techniques involve small solids in contact with hot gases.[ citation needed ]

History

A pyrometer from 1852. Heating the metal bar (a) presses against a lever (b), which moves a pointer (c) along a scale that serves as a measuring index. (e) is an immovable prop which holds the bar in place. A spring on (c) pushes against (b), causing the index to fall back once the bar cools. Pyrometer example.png
A pyrometer from 1852. Heating the metal bar (a) presses against a lever (b), which moves a pointer (c) along a scale that serves as a measuring index. (e) is an immovable prop which holds the bar in place. A spring on (c) pushes against (b), causing the index to fall back once the bar cools.

The earliest example of a pyrometer thought to be in existence is the Hindley Pyrometer held by the London Science Museum, dating from 1752, produced for the Royal collection. The pyrometer was a well known enough instrument that it was described in some detail by the mathematician Euler in 1760. [3]

The potter Josiah Wedgwood invented a different type of pyrometer to measure the temperature in his kilns, [4] which first compared the color of clay fired at known temperatures, but was eventually upgraded to measuring the shrinkage of pieces of clay, which depended on kiln temperature. [5] Later examples used the expansion of a metal bar. [6]

In 1860s-1870s brothers William and Werner Siemens developed a platinum resistance thermometer, initially to measure temperature in undersea cables, but then adapted for measuring temperatures in metallurgy up to 1000 C, hence deserving a name of a pyrometer.

Technician measuring the temperature of molten silicon at 2,650 degF (1,450 degC) with a disappearing-filament pyrometer in Czochralski crystal growing equipment at Raytheon transistor plant in 1956. Silicon grown by Czochralski process 1956.jpg
Technician measuring the temperature of molten silicon at 2,650 °F (1,450 °C) with a disappearing-filament pyrometer in Czochralski crystal growing equipment at Raytheon transistor plant in 1956.

The first disappearing-filament pyrometer was built by L. Holborn and F. Kurlbaum in 1901. [7] This device had a thin electrical filament between an observer's eye and an incandescent object. The current through the filament was adjusted until it was of the same colour (and hence temperature) as the object, and no longer visible; it was calibrated to allow temperature to be inferred from the current. [8]

The temperature returned by the vanishing filament pyrometer and others of its kind, called brightness pyrometers, is dependent on the emissivity of the object. With greater use of brightness pyrometers, it became obvious that problems existed with relying on knowledge of the value of emissivity. Emissivity was found to change, often drastically, with surface roughness, bulk and surface composition, and even the temperature itself. [9]

To get around these difficulties, the ratio or two-color pyrometer was developed. They rely on the fact that Planck's law, which relates temperature to the intensity of radiation emitted at individual wavelengths, can be solved for temperature if Planck's statement of the intensities at two different wavelengths is divided. This solution assumes that the emissivity is the same at both wavelengths [8] and cancels out in the division. This is known as the gray body assumption. Ratio pyrometers are essentially two brightness pyrometers in a single instrument. The operational principles of the ratio pyrometers were developed in the 1920s and 1930s, and they were commercially available in 1939. [7]

As the ratio pyrometer came into popular use, it was determined that many materials, of which metals are an example, do not have the same emissivity at two wavelengths. [10] For these materials, the emissivity does not cancel out and the temperature measurement is in error. The amount of error depends on the emissivities and the wavelengths where the measurements are taken. [8] Two-color ratio pyrometers cannot measure whether a material's emissivity is wavelength dependent.

To more accurately measure the temperature of real objects with unknown or changing emissivities, multiwavelength pyrometers were envisioned at the US National Institute of Standards and Technology and described in 1992. [7] Multiwavelength pyrometers use three or more wavelengths and mathematical manipulation of the results to attempt to achieve accurate temperature measurement even when the emissivity is unknown, changing or differs according to wavelength of measurement. [8] [9] [10]

Applications

A tuyere pyrometer. (1) Display. (2) Optical. (3) Fibre optic cable and periscope. (4) Pyrometer tuyere adapter having: i. Bustle pipe connection. ii. Tuyere clamp. iii. Clamp washer. iv. Clamp stud c/w and fastening hardware. v. Gasket. vi. Noranda tuyere silencer. vii. Valve seat. viii. Ball. (5) Pneumatic cylinder: i. Smart cylinder assembly with Internal proximity switch. ii. Guard plate assembly. iii. Temporary flange cover plate, used to cover periscope entry hole on tuyere adapter when no cylinder is installed on the tuyere. (6) Operator station panel. (7) Pyrometer light station. (8) Limit switches. (9) 4 conductor cab tire. (10) Ball Valve. (11) Periscope air pressure switch. (12) Bustle pipe air pressure switch. (13) Airline filter/regulator. (14) Directional control valve, sub-plate, silencer and speed control mufflers. (15) 2" nom. low pressure air hose, 40m length. Smelter-pyrometer.png
A tuyère pyrometer. (1) Display. (2) Optical. (3) Fibre optic cable and periscope. (4) Pyrometer tuyère adapter having: i. Bustle pipe connection. ii. Tuyère clamp. iii. Clamp washer. iv. Clamp stud c/w and fastening hardware. v. Gasket. vi. Noranda tuyère silencer. vii. Valve seat. viii. Ball. (5) Pneumatic cylinder: i. Smart cylinder assembly with Internal proximity switch. ii. Guard plate assembly. iii. Temporary flange cover plate, used to cover periscope entry hole on tuyère adapter when no cylinder is installed on the tuyère. (6) Operator station panel. (7) Pyrometer light station. (8) Limit switches. (9) 4 conductor cab tire. (10) Ball Valve. (11) Periscope air pressure switch. (12) Bustle pipe air pressure switch. (13) Airline filter/regulator. (14) Directional control valve, sub-plate, silencer and speed control mufflers. (15) 2" nom. low pressure air hose, 40m length.

Pyrometers are suited especially to the measurement of moving objects or any surfaces that cannot be reached or cannot be touched. Contemporary multispectral pyrometers are suitable for measuring high temperatures inside combustion chambers of gas turbine engines with high accuracy. [11]

Temperature is a fundamental parameter in metallurgical furnace operations. Reliable and continuous measurement of the metal temperature is essential for effective control of the operation. Smelting rates can be maximized, slag can be produced at the optimum temperature, fuel consumption is minimized and refractory life may also be lengthened. Thermocouples were the traditional devices used for this purpose, but they are unsuitable for continuous measurement because they melt and degrade.

Measuring the combustion temperature of coke in the blast furnace using an optical pyrometer, Fixed Nitrogen Research Laboratory, 1930. THC 2003.902.127 T. Hignett Optical Pyrometer.tif
Measuring the combustion temperature of coke in the blast furnace using an optical pyrometer, Fixed Nitrogen Research Laboratory, 1930.

Salt bath furnaces operate at temperatures up to 1300 °C and are used for heat treatment. At very high working temperatures with intense heat transfer between the molten salt and the steel being treated, precision is maintained by measuring the temperature of the molten salt. Most errors are caused by slag on the surface which is cooler than the salt bath. [12]

The tuyère pyrometer is an optical instrument for temperature measurement through the tuyeres which are normally used for feeding air or reactants into the bath of the furnace.

A steam boiler may be fitted with a pyrometer to measure the steam temperature in the superheater.

A hot air balloon is equipped with a pyrometer for measuring the temperature at the top of the envelope in order to prevent overheating of the fabric.

Pyrometers may be fitted to experimental gas turbine engines to measure the surface temperature of turbine blades. Such pyrometers can be paired with a tachometer to tie the pyrometer output with the position of an individual turbine blade. Timing combined with a radial position encoder allows engineers to determine the temperature at exact points on blades moving past the probe.

See also

Related Research Articles

<span class="mw-page-title-main">Infrared</span> Form of electromagnetic radiation

Infrared is electromagnetic radiation (EMR) in the spectral band between microwaves and visible light. It is invisible to the human eye. IR is generally understood to encompass wavelengths from around 750 nm to 100 μm.

<span class="mw-page-title-main">Thermometer</span> Device to measure temperature

A thermometer is a device that measures temperature or temperature gradient. A thermometer has two important elements: (1) a temperature sensor in which some change occurs with a change in temperature; and (2) some means of converting this change into a numerical value. Thermometers are widely used in technology and industry to monitor processes, in meteorology, in medicine, and in scientific research.

<span class="mw-page-title-main">Ultraviolet–visible spectroscopy</span> Range of spectroscopic analysis

Ultraviolet (UV) spectroscopy or ultraviolet–visible (UV-VIS) spectrophotometry refers to absorption spectroscopy or reflectance spectroscopy in part of the ultraviolet and the full, adjacent visible regions of the electromagnetic spectrum. Being relatively inexpensive and easily implemented, this methodology is widely used in diverse applied and fundamental applications. The only requirement is that the sample absorb in the UV-Vis region, i.e. be a chromophore. Absorption spectroscopy is complementary to fluorescence spectroscopy. Parameters of interest, besides the wavelength of measurement, are absorbance (A) or transmittance (%T) or reflectance (%R), and its change with time.

<span class="mw-page-title-main">Bolometer</span> Device for measuring incident electromagnetic radiation

A bolometer is a device for measuring radiant heat by means of a material having a temperature-dependent electrical resistance. It was invented in 1878 by the American astronomer Samuel Pierpont Langley.

<span class="mw-page-title-main">Thermal radiation</span> Electromagnetic radiation generated by the thermal motion of particles

Thermal radiation is electromagnetic radiation generated by the thermal motion of particles in matter. Thermal radiation is generated when heat from the movement of charges in the material is converted to electromagnetic radiation. All matter with a temperature greater than absolute zero emits thermal radiation. At room temperature, most of the emission is in the infrared (IR) spectrum. Particle motion results in charge-acceleration or dipole oscillation which produces electromagnetic radiation.

<span class="mw-page-title-main">Thermographic camera</span> Imaging device using infrared radiation

A thermographic camera is a device that creates an image using infrared (IR) radiation, similar to a normal camera that forms an image using visible light. Instead of the 400–700 nanometre (nm) range of the visible light camera, infrared cameras are sensitive to wavelengths from about 1,000 nm to about 14,000 nm (14 μm). The practice of capturing and analyzing the data they provide is called thermography.

<span class="mw-page-title-main">Thermography</span> Use of thermograms to study heat distribution in structures or regions

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<span class="mw-page-title-main">Emissivity</span> Capacity of an object to radiate electromagnetic energy

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<span class="mw-page-title-main">Infrared thermometer</span> Thermometer which infers temperature by measuring infrared energy emission

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<span class="mw-page-title-main">Disappearing-filament pyrometer</span>

The disappearing-filament pyrometer is an optical pyrometer, in which the temperature of a glowing incandescent object is measured by comparing it to the light of a heated filament. Invented independently in 1901 by Ludwig Holborn and Ferdinand Kurlbaum in Germany and Everett Fleet Morse in the United States, it was the first device which could measure temperatures above 1000 °C. Disappearing filament pyrometers have been used to measure temperatures between about 600 °C and 3000 °C. Like other optical pyrometers they are used to measure the temperature of objects too hot for contact thermometers, such as molten metals. Widely used in the steel and ceramics industries as well as for research, they have been almost totally superseded by electronic spectral-band pyrometers.

<span class="mw-page-title-main">Thin filament pyrometry</span>

Thin filament pyrometry (TFP) is an optical method used to measure temperatures. It involves the placement of a thin filament in a hot gas stream. Radiative emissions from the filament can be correlated with filament temperature. Filaments are typically silicon carbide (SiC) fibers with a diameter of 15 micrometres. Temperatures of about 800–2500 K can be measured.

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References

  1. "incandescence". Dictionary.com. Dictionary.com, LLC. Retrieved 2 January 2015.
  2. Coates, P.; Lowe, D. (2016). The Fundamentals of Radiation Thermometers. CRC Press. p. 1. ISBN   978-1-4987-7822-0. Historically the term 'pyrometer' has been widely used. At the present time the term 'radiation thermometer' is more generally favoured.
  3. Euler, Leonhard (1823). Letters of Euler on Different Subjects in Physics and Philosophy, Addressed to a German Princess. With Notes, and a Life of Euler. Translated by Henry Hunter.
  4. "History — Historic Figures: Josiah Wedgwood (1730 - 1795)". BBC. 1970-01-01. Retrieved 2013-08-31.
  5. "Pyrometer". Wedgwood Museum . Retrieved 23 August 2013.
  6. Draper, John William (1861). A Textbook on chemistry. Harper & Bros. p.  24. draper, john william.
  7. 1 2 3 Michalski, L.; Eckersdorf, K.; Kucharski, J.; McGhee, J. (2001). Temperature Measurement. John Wiley & Sons. pp. 162–208. ISBN   978-0-471-86779-1.
  8. 1 2 3 4 Mercer, Carolyn (2003). Optical Metrology for Fluids, Combustion and Solids. Springer Science & Business Media. pp. 297–305. ISBN   978-1-4020-7407-3.
  9. 1 2 Ng, Daniel; Fralick, Gustave (2001). "Use of a multiwavelength pyrometer in several elevated temperature aerospace applications". Review of Scientific Instruments. 72 (2): 1522. Bibcode:2001RScI...72.1522N. doi:10.1063/1.1340558. hdl: 2060/20010035857 . S2CID   52218391.
  10. 1 2 D. Olinger; J. Gray; R. Felice (2007-10-14). Successful Pyrometry in Investment Casting (PDF). Investment Casting Institute 55th Technical Conference and Expo. Investment Casting Institute. Retrieved 2015-04-02.
  11. Mekhrengin, M.V.; Meshkovskii, I.K.; Tashkinov, V.A.; Guryev, V.I.; Sukhinets, A.V.; Smirnov, D.S. (June 2019). "Multispectral pyrometer for high temperature measurements inside combustion chamber of gas turbine engines". Measurement. 139: 355–360. Bibcode:2019Meas..139..355M. doi:10.1016/j.measurement.2019.02.084. S2CID   116260472.
  12. Michalski, L.; Eckersdorf, K.; Kucharski, J.; McGhee, J. (2001). Temperature Measurement. John Wiley & Sons. pp. 403–404. ISBN   978-0-471-86779-1.