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Thermal radiation can be used to detect objects or phenomena normally invisible to the human eye. [[infrared camera|Thermographic cameras]] create an image by sensing infrared radiation. These images can represent the temperature gradient of a scene and are commonly used to locate objects at a higher temperature than their surroundings. In a dark environment where visible light is at low levels, infrared images can be used to locate animals or people due to their body temperature. [[Cosmic microwave background radiation]] is another example of thermal radiation.
 
[[Black-body radiation|Blackbody radiation]] is a concept used to analyze thermal radiation in idealized systems. This model applies if a radiationradiating object meets the physical characteristics of a [[black body]] in [[thermodynamic equilibrium]].<ref name=":8">{{Cite book |last=Huang |first=Kerson |title=Statistical mechanics |date=1987 |publisher=Wiley |isbn=978-0-471-81518-1 |edition=2nd |location=New York}}</ref>{{Rp|page=278}} [[Planck's law]] describes the spectrum of blackbody radiation, and relates the radiative heat flux from a body to its temperature. [[Wien's displacement law]] determines the most likely frequency of the emitted radiation, and the [[Stefan–Boltzmann law]] gives the radiant intensity.<ref name=":8" />{{Rp|page=280}} Where blackbody radiation is not an accurate approximation, emission and absorption can be modeled using [[quantum electrodynamics]] (QED).<ref name=":9" />
 
==Overview==
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=== Renaissance ===
During the same periodRenaissance, [[Santorio Santorio]] came up with one of the earliest [[thermoscope]]s. In 1612 he published his results on the heating effects from the Sun, and his attempts to measure heat from the Moon.<ref name=":4" />
 
Earlier, in 1589, [[Giambattista della Porta]] reported on the heat resentedfelt byon his face, emitted by a remote candle and facilitated by a concave metallic mirror. He also reported the cooling felt from a solid ice block.<ref name=":4" /> Della Porta's experiment would be replicated many times with increasing accuracy. It was replicated by astronomers [[Giovanni Antonio Magini]] and [[Christopher Heydon]] in 1603, and supplied instructions for [[Rudolf II, Holy Roman Emperor]] who performed it in 1611. In 1660, della Porta's experiment was updated by the [[Accademia del Cimento]] using a thermometer invented by [[Ferdinand II, Grand Duke of Tuscany]].<ref name=":4" />
 
=== Enlightenment ===
In 1761, [[Benjamin Franklin]] wrote a letter describing his experiments on the relationship between color and heat absorption.<ref>Cohen, I. B. (1943). [http://www.jstor.org/stable/225739 Franklin’s Experiments on Heat Absorption as a Function of Color] {{Webarchive|url=https://web.archive.org/web/20240925182208/https://www.jstor.org/stable/225739 |date=25 September 2024 }}. ''Isis'', ''34''(5), 404–407.</ref> He found that darker color clothes got hotter when exposed to sunlight than lighter color clothes. One experiment he performed consisted of placing square pieces of cloth of various colorcolors out in the snow on a sunny day. He waited some time and then measured that the black pieces sank furthest into the snow of all the colors, indicating that they got the hottest and melted the most snow.
 
=== Caloric theory ===
{{main|Caloric theory}}
[[Antoine Lavoisier]] considered that radiation of heat was concerned with the condition of the surface of a physical body rather than the material of which it was composed.<ref name=":22">{{Citation |last=Brown |first=Sanborn C. |title=The Caloric Theory |date=1967 |work=Men of Physics: Benjamin Thompson – Count Rumford |pages=16–24 |url=http://dx.doi.org/10.1016/b978-0-08-012179-6.50008-3 |access-date=2021-12-03 |publisher=Elsevier |doi=10.1016/b978-0-08-012179-6.50008-3 |isbn=9780080121796 |archive-date=6 October 2024 |archive-url=https://web.archive.org/web/20241006084656/https://www.sciencedirect.com/unsupported_browser |url-status=live }}</ref> Lavoisier described a poor radiator to be a substance with a polished or smooth surface as it possessed its molecules lying in a plane closely bound together thus creating a surface layer of caloric fluid which insulated the release of the rest within.<ref name=":22" /> He described a greatgood radiator to be a substance with a rough surface as only a small amountproportion of molecules held caloric in within a given plane, allowing for greater escape from within.<ref name=":22" /> [[Benjamin Thompson|Count Rumford]] would later cite this explanation of caloric movement as insufficient to explain the radiation of cold, becomingwhich became a point of contention for the theory as a whole.<ref name=":22" />
 
In his first memoir, [[Augustin-Jean Fresnel]] responded to a view he extracted from a French translation of [[Isaac Newton]]'s ''[[Optics]]''. He says that Newton imagined particles of light traversing space uninhibited by the caloric medium filling it, and refutes this view (never actually held by Newton) by saying that a body under illumination would increase indefinitely in heat.<ref>{{cite book |last=Gillispie |first=Charles Coulston |url=https://archive.org/details/edgeofobjectivit00char/page/408 |title=The Edge of Objectivity: An Essay in the History of Scientific Ideas |publisher=Princeton University Press |year=1960 |isbn=0-691-02350-6 |pages=[https://archive.org/details/edgeofobjectivit00char/page/408 408–9] |author-link1=Charles Coulston Gillispie |url-access=registration}}</ref>
 
In [[Marc-Auguste Pictet]]'s famous [[Pictet's experiment|experiment of 1790]], it was reported that a thermometer detected a lower temperature when a set of mirrormirrors were used to focus "frigorific rays" from a cold object.<ref>{{Cite book |last1=Lemons |first1=Don S. |url=https://books.google.com/books?id=fUpTEAAAQBAJ |title=On the Trail of Blackbody Radiation: Max Planck and the Physics of his Era |last2=Shanahan |first2=William R. |last3=Buchholtz |first3=Louis J. |date=2022-09-20 |publisher=MIT Press |isbn=978-0-262-04704-3 |language=en |access-date=29 February 2024 |archive-date=6 October 2024 |archive-url=https://web.archive.org/web/20241006084643/https://books.google.com/books?id=fUpTEAAAQBAJ |url-status=live }}</ref>
 
In 1791, [[Pierre Prevost (physicist)|Pierre Prevost]] a colleague of Pictet, introduced the concept of [[radiative equilibrium]], wherein all objects both radiatesradiate and absorb heat.<ref name=":5">{{Cite web |title=Pierre Prévost |url=https://www.oxfordreference.com/display/10.1093/oi/authority.20110803100344451 |access-date=2024-02-29 |website=Oxford Reference |language=en |archive-date=6 October 2024 |archive-url=https://web.archive.org/web/20241006084644/https://www.oxfordreference.com/display/10.1093/oi/authority.20110803100344451 |url-status=live }}</ref> When an object is cooler than its surroundings, it absorbs more heat than it emits, causing its temperature to increase until it reaches equilibrium. Even at equilibrium, it continues to radiate heat, balancing absorption and emission.<ref name=":5" />
 
The discovery of infrared radiation is ascribed to astronomer [[William Herschel]]. Herschel published his results in 1800 before the [[Royal Society of London]]. Herschel used a [[Triangular prism (optics)|prism]] to [[refract]] light from the [[sun]] and detected the calorific rays, beyond the [[red]] part of the spectrum, asby an increase in the temperature recorded on a [[thermometer]] in that region.<ref>{{cite journal |last=Herschel |first=William |year=1800 |title=Experiments on the refrangibility of the invisible rays of the Sun |url=https://babel.hathitrust.org/cgi/pt?id=pst.000054592520;view=1up;seq=358 |journal=Philosophical Transactions of the Royal Society of London |volume=90 |pages=284–292 |doi=10.1098/rstl.1800.0015 |jstor=107057 |doi-access=free |access-date=1 March 2024 |archive-date=4 February 2021 |archive-url=https://web.archive.org/web/20210204133019/https://babel.hathitrust.org/cgi/pt?id=pst.000054592520;view=1up;seq=358 |url-status=live }}</ref><ref>{{cite web |title=Herschel Discovers Infrared Light |url=http://coolcosmos.ipac.caltech.edu/cosmic_classroom/classroom_activities/herschel_bio.html |url-status=dead |archive-url=https://web.archive.org/web/20120225094516/http://coolcosmos.ipac.caltech.edu/cosmic_classroom/classroom_activities/herschel_bio.html |archive-date=2012-02-25 |access-date=2011-11-08 |website=Coolcosmos.ipac.caltech.edu}}</ref>
 
=== AetherElectromagnetic theory ===
First,At the earlierend theory which originated fromof the concept19th ofcentury ait hypotheticalwas mediumshown referredthat as [[Luminiferous aether|aether]]. Ether supposedly fills all evacuated or non-evacuated spaces. Thethe transmission of light or of [[radiant heat]] arewas allowed by the propagation of [[electromagnetic waves]] in the aether.<ref name="hsu">Hsu, Shao Ti. ''Engineering Heat Transfer''. Blacksburg, Virginia:D. Van Nostrand Company, Inc.,1962.</ref> [[televisionTelevision]] and [[radio]] broadcasting waves are types of electromagnetic waves with specific [[wavelengths]].<ref name="becker">Becker, Martin. ''Heat Transfer a Modern Approach'' New York: Plenum Publishing Corporation, 1986.</ref> All [[electromagnetic waves]] travel at the same speed; therefore, shorter [[wavelengths]] are associated with high frequencies. Since every body or fluid is submerged in the ether, due to the vibration of the molecules, any body or fluid can potentially initiate an electromagnetic wave. All bodies generate and receive electromagnetic waves at the expense of its storedheat energyexchange.<ref name="becker" />
{{See also|Aether theories}}
First, the earlier theory which originated from the concept of a hypothetical medium referred as [[Luminiferous aether|aether]]. Ether supposedly fills all evacuated or non-evacuated spaces. The transmission of light or of [[radiant heat]] are allowed by the propagation of [[electromagnetic waves]] in the aether.<ref name="hsu">Hsu, Shao Ti. ''Engineering Heat Transfer''. Blacksburg, Virginia:D. Van Nostrand Company, Inc.,1962.</ref> [[television]] and [[radio]] broadcasting waves are types of electromagnetic waves with specific [[wavelengths]].<ref name="becker">Becker, Martin. ''Heat Transfer a Modern Approach'' New York: Plenum Publishing Corporation, 1986.</ref> All [[electromagnetic waves]] travel at the same speed; therefore, shorter [[wavelengths]] are associated with high frequencies. Since every body or fluid is submerged in the ether, due to the vibration of the molecules, any body or fluid can potentially initiate an electromagnetic wave. All bodies generate and receive electromagnetic waves at the expense of its stored energy.<ref name="becker" />
 
In 1860, [[Gustav Kirchhoff]] published a mathematical description of [[thermal equilibrium]] (i.e. [[Kirchhoff's law of thermal radiation]]).<ref name=":7" />{{Rp|pages=275–301}} By 1884 the emissive power of a perfect blackbody was inferred by [[Josef Stefan]] using [[John Tyndall]]'s experimental measurements, and derived by [[Ludwig Boltzmann]] from fundamental statistical principles.<ref>{{cite journal |last1=Boltzmann |first1=Ludwig |date=1884 |title=Ableitung des Stefan'schen Gesetzes, betreffend die Abhängigkeit der Wärmestrahlung von der Temperatur aus der electromagnetischen Lichttheorie |trans-title=Derivation of Stefan's law, concerning the dependency of heat radiation on temperature, from the electromagnetic theory of light |url=https://babel.hathitrust.org/cgi/pt?id=uc1.a0002763670;view=1up;seq=305 |journal=Annalen der Physik und Chemie |language=de |volume=258 |issue=6 |pages=291–294 |bibcode=1884AnP...258..291B |doi=10.1002/andp.18842580616 |doi-access=free |access-date=25 March 2024 |archive-date=29 July 2020 |archive-url=https://web.archive.org/web/20200729024251/https://babel.hathitrust.org/cgi/pt?id=uc1.a0002763670 |url-status=live }}</ref> This relation is known as [[Stefan–Boltzmann law]].