Black-body radiation, shipping iron and steel products via the Black Warrior River through the Panama Canal to the West Coast of the United States and the world. High-grade coal is barged to Mobile and is then shipped throughout the world, making Mobile the largest coal port in the Southeastern states. Coal mining and production in west-central Alabama is one of the larger employers and is likely to continue being important to the energy needs of the world. Today, a severe threat to the Black Warrior River is sedimentation, or siltation, the primary causes of which are development projects, logging and 	Black Warrior River
7680792	mining operations, and the building and maintaining of roads. Black Warrior River The Black Warrior River is a waterway in west-central Alabama in the southeastern United States. The river rises in the extreme southern edges of the Appalachian Highlands and flows 178 miles (286 km) to the Tombigbee River, of which the Black Warrior is the primary tributary. The river is named after the Mississippian paramount chief Tuskaloosa, whose name was Muskogean for 'Black Warrior'. The Black Warrior is impounded along nearly its entire course by a series of locks and dams to form a chain of reservoirs that 	Black Warrior River
7680793	Massachusetts Route 79 Massachusetts Route 79 Route 79 is a state highway in southeastern Massachusetts. The route begins as a highway in Fall River also known as the Fall River Viaduct and Western Fall River Expressway before becoming a more rural route. Route description. Route 79 begins south of the Braga Bridge and I-195, multiplexed with Route 138 as a surface four-lane controlled-access highway. It has exits to Davol Street, which act as one-way frontage roads on both sides of Route 79, and to the Veterans Memorial Bridge, at which point Route 138 leaves Route 79 and goes over the 	Massachusetts Route 79
7680794	bridge. The route continues northward, passing under North Main Street with exit access to that street. It then connects to Route 24 at that route's exit 7. There is no access between Route 79 north and Route 24 south, or vice versa. The route continues concurrently along Route 24 into the Assonet section of the town of Freetown, where it leaves its concurrency at exit 11 (formerly 9), turning on to South Main Street. (South Main Street southbound in Assonet connects to North Main Street in Fall River.) The route passes through the village before turning eastward along Elm 	Massachusetts Route 79
7680795	Street, intertwining with the Assonet River as both make their way into Berkley. In Berkley, Route 79 passes through the village of Myricks, in the far eastern end of the town. It crosses the Old Colony Railroad lines and County Road, the former alignment of Route 140, before crossing the current route at Exit 16 (formerly 10) just over the Taunton line. In Taunton, the route follows along the Taunton-Lakeville town line before leaving Taunton completely. In Lakeville, the route heads through the northern part of the town, crossing Route 18 and passing the former Lakeville Hospital, before ending 	Massachusetts Route 79
7680796	at a 4-way intersection with Route 105 and Commercial Drive, the main road which leads to the Middleborough/Lakeville MBTA station. History. In 2012, the northern terminus of Route 79 was relocated. Before the project, the northern terminus of Route 79 still ended at Route 105, only 1/10 of a mile north of its current terminus, but it was too close to the southbound ramps for Interstate 495. By relocating Route 79 to a four-way intersection with Route 105 and Commercial Drive, traffic was eased during rush hour. Instead of Route 79 traffic looping onto Route 105 to 	Massachusetts Route 79
7680797	get to the MBTA station, the new alignment provides easier access to the MBTA station from areas such as North Lakeville, East Taunton, Berkley and Freetown. The southern end of Route 79 used to be a double-decked elevated highway called the Fall River Viaduct, with ramps to Route 138 and I-195. The viaduct continued northward under the Braga Bridge for a third of a mile before splitting into a surface four-lane highway. As part of a $3 billion effort to replace structurally deficient bridges in Massachusetts, the Massachusetts Department of Transportation replaced the Fall River Viaduct and 	Massachusetts Route 79
7680798	some of its connector ramps to I-195 with new roadways and structures. The project was completed in 2016. Major intersections. All interchanges south of Route 24 are unnumbered. Massachusetts Route 79 Route 79 is a state highway in southeastern Massachusetts. The route begins as a highway in Fall River also known as the Fall River Viaduct and Western Fall River Expressway before becoming a more rural route. Route description. Route 79 begins south of the Braga Bridge and I-195, multiplexed with Route 138 as a surface four-lane controlled-access highway. It has exits to Davol Street, which act as 	Massachusetts Route 79
7680799	Glen Bell Glen Bell Glen William Bell Jr. (September 3, 1923 – January 16, 2010) was an American entrepreneur who founded the Taco Bell chain of restaurants. Biography. Glen Bell was born in Lynwood, California, to Glen William Bell Sr. and Ruth Elizabeth Bell (née Johnson). His parents were born in the Midwest with his mother having been born in Kandiyohi County, Minnesota and his father in Franklin County, Iowa. Bell's mother Ruth was born to a half Swedish father and a predominantly English mother. His father Glen Sr. was born to a German father and predominantly English mother, Glen also had 	Glen Bell
7680800	colonial New England ancestry through both his parents families. Bell graduated from San Bernardino High School in 1941. He served in the U.S. Marine Corps as a cook during World War II. After the Marines he started his first hot dog stand 'Bell's Drive-In', in San Bernardino in 1948. In 1952, he sold the hot dog stand and built a second location selling hot dogs and hamburgers. He soon started selling tacos at a taco stand named Taco-Tia at 19 cents each from a side window. Between 1954 and 1955, he opened three Taco Tias in the 	Glen Bell
7680801	San Bernardino area, eventually selling those restaurants and opening four El Tacos with a partner in the Long Beach area. Glen Bell learned how to make tacos from the Mitla Café in San Bernardino. In 1962, he went solo and sold the El Tacos to his partner and opened his first Taco Bell in Downey, California. Bell franchised his restaurant in 1964. His company grew rapidly, and the 868-restaurant chain was later sold to PepsiCo in 1978 for $125 million in stock. West Side and Cherry Valley Railroad. In the late 1970s, Bell opened a tourist railroad at 	Glen Bell
7680802	Tuolumne, California. This gauge railroad used the lower section of the track and several steam locomotives of the West Side Lumber Company railway. The operation offered boat rides on the old mill pond and RV parking. In the initial plan, there were themed areas of the park with restaurants and stores. Glen Bell was able to locate and purchase old equipment (trains, cars, water towers, etc.) that were used in logging operations and brought to the park. It closed in the early 1980s after failing traffic. The property was eventually sold off to the Tuolumne tribe of the Mi Wuk 	Glen Bell
7680803	Indians who have developed the land including event grounds that have hosted big name concerts including Pat Benatar, Melissa Etheridge, Smokey Robinson, Peter Frampton, Bad Company and other touring acts. Death. Bell died from Parkinson's disease on January 16, 2010, at age 86 in Rancho Santa Fe, California, leaving his wife, Martha, two sons, two daughters, four grandchildren, and three sisters. Glen Bell Glen William Bell Jr. (September 3, 1923 – January 16, 2010) was an American entrepreneur who founded the Taco Bell chain of restaurants. Biography. Glen Bell was born in Lynwood, California, to Glen William Bell Sr. and 	Glen Bell
7680804	Black-body radiation Black-body radiation Black-body radiation is the thermal electromagnetic radiation within or surrounding a body in thermodynamic equilibrium with its environment, emitted by a black body (an idealized opaque, non-reflective body). It has a specific, continuous, spectrum of wavelengths, inversely related to intensity that depend only on the body's temperature, which is assumed for the sake of calculations and theory to be uniform and constant. A perfectly insulated enclosure that is in thermal equilibrium internally contains black-body radiation and will emit it through a hole made in its wall, provided the hole is small enough to 	Black-body radiation
7680805	have a negligible effect upon the equilibrium. The thermal radiation spontaneously emitted by many ordinary objects can be approximated as black-body radiation. Of particular importance, although planets and stars (including our own sun) are neither in thermal equilibrium with their surroundings nor perfect black bodies, black-body radiation is a good first approximation for the energy they emit, which after being filtered by the earths atmosphere thus characterises daylight", which humans (also most other animals) have evolved to use for vision. A black body at room temperature radiates only in the infrared spectrum and cannot be perceived by  the human eye, but some reptiles can sense. As the object becomes a little hotter, the emission spectrum gets stronger and extends into the human visual range and the object appears dull red, and as its temperature increases further it emits more and more orange, yellow, green, blue light, (and ultimately beyond violet). Note that while "daylight" (sunlight) is approximately a continuous black body spectrum (filtered by the atmosphere), what humans (also colour film and camera sensors) perceive as "white" light is NOT a continuous spectrum, rather is an illusion based on the relative mixture of light stimulating separate red , green and blue photoreceptors in the eye/colour film/camera sensors etc., in a ratio approximating a black body emission at a certain "colour temperature" (e.g. daylight being the surface of the sun, around 5-6,000K). E.g. Tungsten filament lights have a continuous black body spectrum with a cooler colour temperature around 2,700K, which also emits considerable energy in the infra red range, but today's more efficient fluorescent and LED lighting use do NOT have a continuous black body emission spectrum, rather emit directly or use combinations of phosphors that emit narrow spectrums. Black holes are near -perfect black bodies, in the sense that they absorb all the radiation that falls on them. It has been proposed that they emit black-body radiation (called Hawking radiation), with a temperature that depends on the mass of the black hole. The term "black body" was introduced by Gustav Kirchhoff in 1860. Black-body radiation is also called thermal radiation, "cavity radiation", "complete radiation" or "temperature radiation". Theory. Spectrum. Black-body radiation has a characteristic, continuous frequency spectrum that depends only on the body's temperature, called the Planck spectrum or Planck's law. The spectrum is peaked at a  characteristic frequency that shifts to higher frequencies with increasing temperature, and at room temperature most of the emission is in the infrared region of the electromagnetic spectrum. As the temperature increases past about 500 degrees Celsius, black bodies start to emit significant amounts of visible light. Viewed in the dark by the human eye, the first faint glow appears as a "ghostly" grey (the visible light is actually red, but low intensity light activates only the eye's grey-level sensors). With rising temperature, the glow becomes visible even when there is some background surrounding light: first as a dull  red, then yellow, and eventually a "dazzling bluish-white" as the temperature rises. When the body appears white, it is emitting a substantial fraction of its energy as ultraviolet radiation. The Sun, with an effective temperature of approximately 5800 K, is an approximate black body with an emission spectrum peaked in the central, yellow-green part of the visible spectrum, but with significant power in the ultraviolet as well. Black-body radiation provides insight into the thermodynamic equilibrium state of cavity radiation. Black body. All normal (baryonic) matter emits electromagnetic radiation when it has a temperature above absolute zero. The  radiation represents a conversion of a body's internal energy into electromagnetic energy, and is therefore called thermal radiation. It is a spontaneous process of radiative distribution of entropy. Conversely, all normal matter absorbs electromagnetic radiation to some degree. An object that absorbs all radiation falling on it, at all wavelengths, is called a black body. When a black body is at a uniform temperature, its emission has a characteristic frequency distribution that depends on the temperature. Its emission is called black-body radiation. The concept of the black body is an idealization, as perfect black bodies do not exist  in nature. Graphite and lamp black, with emissivities greater than 0.95, however, are good approximations to a black material. Experimentally, black-body radiation may be established best as the ultimately stable steady state equilibrium radiation in a cavity in a rigid body, at a uniform temperature, that is entirely opaque and is only partly reflective. A closed box with walls of graphite at a constant temperature with a small hole on one side produces a good approximation to ideal black-body radiation emanating from the opening. Black-body radiation has the unique absolutely stable distribution of radiative intensity that can  persist in thermodynamic equilibrium in a cavity. In equilibrium, for each frequency the total intensity of radiation that is emitted and reflected from a body (that is, the net amount of radiation leaving its surface, called the "spectral radiance") is determined solely by the equilibrium temperature and does not depend upon the shape, material or structure of the body. For a black body (a perfect absorber) there is no reflected radiation, and so the spectral radiance is entirely due to emission. In addition, a black body is a diffuse emitter (its emission is independent of direction). Consequently, black-body radiation  may be viewed as the radiation from a black body at thermal equilibrium. Black-body radiation becomes a visible glow of light if the temperature of the object is high enough. The Draper point is the temperature at which all solids glow a dim red, about . At , a small opening in the wall of a large uniformly heated opaque-walled cavity (such as an oven), viewed from outside, looks red; at , it looks white. No matter how the oven is constructed, or of what material, as long as it is built so that almost all light entering is absorbed by  its walls, it will contain a good approximation to black-body radiation. The spectrum, and therefore color, of the light that comes out will be a function of the cavity temperature alone. A graph of the amount of energy inside the oven per unit volume and per unit frequency interval plotted versus frequency is called the "black-body curve". Different curves are obtained by varying the temperature. Two bodies that are at the same temperature stay in mutual thermal equilibrium, so a body at temperature "T" surrounded by a cloud of light at temperature "T" on average will emit as  much light into the cloud as it absorbs, following Prevost's exchange principle, which refers to radiative equilibrium. The principle of detailed balance says that in thermodynamic equilibrium every elementary process works equally in its forward and backward sense. Prevost also showed that the emission from a body is logically determined solely by its own internal state. The causal effect of thermodynamic absorption on thermodynamic (spontaneous) emission is not direct, but is only indirect as it affects the internal state of the body. This means that at thermodynamic equilibrium the amount of every wavelength in every direction of thermal radiation  emitted by a body at temperature "T", black or not, is equal to the corresponding amount that the body absorbs because it is surrounded by light at temperature "T". When the body is black, the absorption is obvious: the amount of light absorbed is all the light that hits the surface. For a black body much bigger than the wavelength, the light energy absorbed at any wavelength "λ" per unit time is strictly proportional to the black-body curve. This means that the black-body curve is the amount of light energy emitted by a black body, which justifies the  name. This is the condition for the applicability of Kirchhoff's law of thermal radiation: the black-body curve is characteristic of thermal light, which depends only on the temperature of the walls of the cavity, provided that the walls of the cavity are completely opaque and are not very reflective, and that the cavity is in thermodynamic equilibrium. When the black body is small, so that its size is comparable to the wavelength of light, the absorption is modified, because a small object is not an efficient absorber of light of long wavelength, but the principle of strict equality  of emission and absorption is always upheld in a condition of thermodynamic equilibrium. In the laboratory, black-body radiation is approximated by the radiation from a small hole in a large cavity, a hohlraum, in an entirely opaque body that is only partly reflective, that is maintained at a constant temperature. (This technique leads to the alternative term "cavity radiation".) Any light entering the hole would have to reflect off the walls of the cavity multiple times before it escaped, in which process it is nearly certain to be absorbed. Absorption occurs regardless of the wavelength of the radiation entering  (as long as it is small compared to the hole). The hole, then, is a close approximation of a theoretical black body and, if the cavity is heated, the spectrum of the hole's radiation (i.e., the amount of light emitted from the hole at each wavelength) will be continuous, and will depend only on the temperature and the fact that the walls are opaque and at least partly absorptive, but not on the particular material of which they are built nor on the material in the cavity (compare with emission spectrum). The radiance or observed intensity is not a  function of direction. Therefore, a black body is a perfect Lambertian radiator. Real objects never behave as full-ideal black bodies, and instead the emitted radiation at a given frequency is a fraction of what the ideal emission would be. The emissivity of a material specifies how well a real body radiates energy as compared with a black body. This emissivity depends on factors such as temperature, emission angle, and wavelength. However, it is typical in engineering to assume that a surface's spectral emissivity and absorptivity do not depend on wavelength so that the emissivity is a constant. This  is known as the "gray body" assumption. With non-black surfaces, the deviations from ideal black-body behavior are determined by both the surface structure, such as roughness or granularity, and the chemical composition. On a "per wavelength" basis, real objects in states of local thermodynamic equilibrium still follow Kirchhoff's Law: emissivity equals absorptivity, so that an object that does not absorb all incident light will also emit less radiation than an ideal black body; the incomplete absorption can be due to some of the incident light being transmitted through the body or to some of it being reflected  at the surface of the body. In astronomy, objects such as stars are frequently regarded as black bodies, though this is often a poor approximation. An almost perfect black-body spectrum is exhibited by the cosmic microwave background radiation. Hawking radiation is the hypothetical black-body radiation emitted by black holes, at a temperature that depends on the mass, charge, and spin of the hole. If this prediction is correct, black holes will very gradually shrink and evaporate over time as they lose mass by the emission of photons and other particles. A black body radiates energy at all frequencies , but its intensity rapidly tends to zero at high frequencies (short wavelengths). For example, a black body at room temperature () with one square meter of surface area will emit a photon in the visible range (390–750 nm) at an average rate of one photon every 41 seconds, meaning that, for most practical purposes, such a black body does not emit in the visible range. The study of the laws of black bodies and the failure of classical physics to describe them helped establish the foundations of quantum mechanics. Further explanation. According to the Classical Theory of Radiation, if each Fourier  mode of the equilibrium radiation (in an otherwise empty cavity with perfectly reflective walls) is considered as a degree of freedom capable of exchanging energy, then, according to the equipartition theorem of classical physics, there would be an equal amount of energy in each mode. Since there are an infinite number of modes, this would imply infinite heat capacity, as well as a nonphysical spectrum of emitted radiation that grows without bound with increasing frequency, a problem known as the ultraviolet catastrophe. In the longer wavelengths this deviation is not so noticeable, as formula_1 and formula_2 are very small. In  the shorter wavelengths of the ultraviolet range, however, classical theory predicts the energy emitted tends to infinity, hence the ultraviolet catastrophe. The theory even predicted that all bodies would emit most of their energy in the ultraviolet range, clearly contradicted by the experimental data which showed a different peak wavelength at different temperatures (see also Wien's law). Instead, in the quantum treatment of this problem, the numbers of the energy modes are quantized, attenuating the spectrum at high frequency in agreement with experimental observation and resolving the catastrophe. The modes that had more energy than the thermal energy of  the substance itself were not considered, and because of quantization modes having infinitesimally little energy were excluded. Thus for shorter wavelengths very few modes (having energy more than formula_1) were allowed, supporting the data that the energy emitted is reduced for wavelengths less than the wavelength of the observed peak of emission. Notice that there are two factors responsible for the shape of the graph. Firstly, longer wavelengths have a larger number of modes associated with them. Secondly, shorter wavelengths have more energy associated per mode. The two factors combined give the characteristic maximum wavelength. Calculating the black-body curve  was a major challenge in theoretical physics during the late nineteenth century. The problem was solved in 1901 by Max Planck in the formalism now known as Planck's law of black-body radiation. By making changes to Wien's radiation law (not to be confused with Wien's displacement law) consistent with thermodynamics and electromagnetism, he found a mathematical expression fitting the experimental data satisfactorily. Planck had to assume that the energy of the oscillators in the cavity was quantized, i.e., it existed in integer multiples of some quantity. Einstein built on this idea and proposed the quantization of  electromagnetic radiation itself in 1905 to explain the photoelectric effect. These theoretical advances eventually resulted in the superseding of classical electromagnetism by quantum electrodynamics. These quanta were called photons and the black-body cavity was thought of as containing a gas of photons. In addition, it led to the development of quantum probability distributions, called Fermi–Dirac statistics and Bose–Einstein statistics, each applicable to a different class of particles, fermions and bosons. The wavelength at which the radiation is strongest is given by Wien's displacement law, and the overall power emitted per unit area is given by the  Stefan–Boltzmann law. So, as temperature increases, the glow color changes from red to yellow to white to blue. Even as the peak wavelength moves into the ultra-violet, enough radiation continues to be emitted in the blue wavelengths that the body will continue to appear blue. It will never become invisible—indeed, the radiation of visible light increases monotonically with temperature. The Stefan–Boltzmann law also says that the total radiant heat energy emitted from a surface is proportional to the fourth power of its absolute temperature. The law was formulated by Josef Stefan in 1879 and later derived  by Ludwig Boltzmann. The formula is given, where "E" is the radiant heat emitted from a unit of area per unit time, "T" is the absolute temperature, and is the Stefan–Boltzmann constant. Equations. Planck's law of black-body radiation. Planck's law states that where For a black body surface, the spectral radiance density (defined per unit of area normal to the propagation) is independent of the angle formula_13 of emission with respect to the normal. However, this means that, following Lambert's cosine law, formula_14 is the radiance density per unit area of emitting surface as the  surface area involved in generating the radiance is increased by a factor formula_15 with respect to an area normal to the propagation direction. At oblique angles, the solid angle spans involved do get smaller, resulting in lower aggregate intensities. Wien's displacement law. Wien's displacement law shows how the spectrum of black-body radiation at any temperature is related to the spectrum at any other temperature. If we know the shape of the spectrum at one temperature, we can calculate the shape at any other temperature. Spectral intensity can be expressed as a function of wavelength or of frequency . A consequence of Wien's displacement law is that the wavelength at which the intensity "per unit wavelength" of the radiation produced by a black body has a local maximum or peak, formula_16, is a function only of the temperature: where the constant "b", known as Wien's displacement constant, is equal to formula_18 (where formula_19 is the Lambert W function), approximately . At a typical room temperature of 293 K (20 °C), the maximum intensity is at . Planck's law was also stated above as a function of frequency. The intensity maximum for this is given by In unitless  form, the maximum occurs when formula_21, where formula_22. The approximate numerical solution is formula_23. At a typical room temperature of 293 K (20 °C), the maximum intensity is for . Stefan–Boltzmann law. By integrating formula_24 over the frequency the radiance formula_25 (units: power / [area * solid angle] ) is by using formula_27 with formula_28 and with formula_29 being the Stefan–Boltzmann constant. On a side note, at a distance d, the intensity formula_30 per area formula_31 of radiating surface is the useful expression when the receiving surface is perpendicular to the radiation. By subsequently integrating formula_25 over the solid angle formula_34  for all azimuthal angle (0 to formula_35) and polar angle formula_13 from 0 to formula_37, we arrive at the Stefan–Boltzmann law: the power "j"* emitted per unit area of the surface of a black body is directly proportional to the fourth power of its absolute temperature: We used Applications. Human-body emission. The human body radiates energy as infrared light. The net power radiated is the difference between the power emitted and the power absorbed: Applying the Stefan–Boltzmann law, where "A" and "T" are the body surface area and temperature, formula_42 is the emissivity, and "T" is the  ambient temperature. The total surface area of an adult is about 2 m, and the mid- and far-infrared emissivity of skin and most clothing is near unity, as it is for most nonmetallic surfaces. Skin temperature is about 33 °C, but clothing reduces the surface temperature to about 28 °C when the ambient temperature is 20 °C. Hence, the net radiative heat loss is about The total energy radiated in one day is about 8 MJ, or 2000 kcal (food calories). Basal metabolic rate for a 40-year-old male is about 35 kcal/(m·h), which is  equivalent to 1700 kcal per day, assuming the same 2 m area. However, the mean metabolic rate of sedentary adults is about 50% to 70% greater than their basal rate. There are other important thermal loss mechanisms, including convection and evaporation. Conduction is negligible – the Nusselt number is much greater than unity. Evaporation by perspiration is only required if radiation and convection are insufficient to maintain a steady-state temperature (but evaporation from the lungs occurs regardless). Free-convection rates are comparable, albeit somewhat lower, than radiative rates. Thus, radiation accounts for about two-thirds of thermal energy loss in  cool, still air. Given the approximate nature of many of the assumptions, this can only be taken as a crude estimate. Ambient air motion, causing forced convection, or evaporation reduces the relative importance of radiation as a thermal-loss mechanism. Application of Wien's law to human-body emission results in a peak wavelength of For this reason, thermal imaging devices for human subjects are most sensitive in the 7–14 micrometer range. Temperature relation between a planet and its star. The black-body law may be used to estimate the temperature of a planet orbiting the Sun. The temperature of  a planet depends on several factors: The analysis only considers the Sun's heat for a planet in a Solar System. The Stefan–Boltzmann law gives the total power (energy/second) the Sun is emitting: where The Sun emits that power equally in all directions. Because of this, the planet is hit with only a tiny fraction of it. The power from the Sun that strikes the planet (at the top of the atmosphere) is: where Because of its high temperature, the Sun emits to a large extent in the ultraviolet and visible (UV-Vis) frequency range. In this frequency  range, the planet reflects a fraction formula_52 of this energy where formula_52 is the albedo or reflectance of the planet in the UV-Vis range. In other words, the planet absorbs a fraction formula_54 of the Sun's light, and reflects the rest. The power absorbed by the planet and its atmosphere is then: Even though the planet only absorbs as a circular area formula_56, it emits in all directions; the spherical surface area being formula_57. If the planet were a perfect black body, it would emit according to the Stefan–Boltzmann law where formula_59 is the temperature of the  planet. This temperature, calculated for the case of the planet acting as a black body by setting formula_60, is known as the effective temperature. The actual temperature of the planet will likely be different, depending on its surface and atmospheric properties. Ignoring the atmosphere and greenhouse effect, the planet, since it is at a much lower temperature than the Sun, emits mostly in the infrared (IR) portion of the spectrum. In this frequency range, it emits formula_61 of the radiation that a black body would emit where formula_61 is the average emissivity in the IR range. The power emitted by  the planet is then: For a body in radiative exchange equilibrium with its surroundings, the rate at which it emits radiant energy is equal to the rate at which it absorbs it: Substituting the expressions for solar and planet power in equations 1–6 and simplifying yields the estimated temperature of the planet, ignoring greenhouse effect, "T": In other words, given the assumptions made, the temperature of a planet depends only on the surface temperature of the Sun, the radius of the Sun, the distance between the planet and the Sun, the albedo and the IR emissivity of the planet. Notice  that a gray (flat spectrum) ball where formula_66 comes to the same temperature as a black body no matter how dark or light gray . Effective temperature of Earth. Substituting the measured values for the Sun and Earth yields: With the average emissivity formula_71 set to unity, the effective temperature of the Earth is: or −18.8 °C. This is the temperature of the Earth if it radiated as a perfect black body in the infrared, assuming an unchanging albedo and ignoring greenhouse effects (which can raise the surface temperature of a body above what it would be if it were  a perfect black body in all spectrums). The Earth in fact radiates not quite as a perfect black body in the infrared which will raise the estimated temperature a few degrees above the effective temperature. If we wish to estimate what the temperature of the Earth would be if it had no atmosphere, then we could take the albedo and emissivity of the Moon as a good estimate. The albedo and emissivity of the Moon are about 0.1054 and 0.95 respectively, yielding an estimated temperature of about 1.36 °C. Estimates of the Earth's average albedo vary in the  range 0.3–0.4, resulting in different estimated effective temperatures. Estimates are often based on the solar constant (total insolation power density) rather than the temperature, size, and distance of the Sun. For example, using 0.4 for albedo, and an insolation of 1400 W m, one obtains an effective temperature of about 245 K. Similarly using albedo 0.3 and solar constant of 1372 W m, one obtains an effective temperature of 255 K. Cosmology. The cosmic microwave background radiation observed today is the most perfect black-body radiation ever observed in nature, with a temperature of about 2.7 K. It is a  snapshot of the radiation at the time of decoupling between matter and radiation in the early universe. Prior to this time, most matter in the universe was in the form of an ionized plasma in thermal, though not full thermodynamic, equilibrium with radiation. According to Kondepudi and Prigogine, at very high temperatures (above 10 K; such temperatures existed in the very early universe), where the thermal motion separates protons and neutrons in spite of the strong nuclear forces, electron-positron pairs appear and disappear spontaneously and are in thermal equilibrium with electromagnetic radiation. These particles form a part of the  black body spectrum, in addition to the electromagnetic radiation. History. In his first memoir, Augustin-Jean Fresnel (1788–1827) 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 black body under illumination would increase indefinitely in heat. Balfour Stewart. In 1858, Balfour Stewart described his experiments on the thermal radiative emissive and absorptive powers of polished plates of various substances, compared with the powers of  lamp-black surfaces, at the same temperature. Stewart chose lamp-black surfaces as his reference because of various previous experimental findings, especially those of Pierre Prevost and of John Leslie. He wrote, "Lamp-black, which absorbs all the rays that fall upon it, and therefore possesses the greatest possible absorbing power, will possess also the greatest possible radiating power." More an experimenter than a logician, Stewart failed to point out that his statement presupposed an abstract general principle: that there exist, either ideally in theory, or really in nature, bodies or surfaces that respectively have one and the same unique  universal greatest possible absorbing power, likewise for radiating power, for every wavelength and equilibrium temperature. Stewart measured radiated power with a thermopile and sensitive galvanometer read with a microscope. He was concerned with selective thermal radiation, which he investigated with plates of substances that radiated and absorbed selectively for different qualities of radiation rather than maximally for all qualities of radiation. He discussed the experiments in terms of rays which could be reflected and refracted, and which obeyed the Stokes-Helmholtz reciprocity principle (though he did not use an eponym for it). He did not in this paper mention that  the qualities of the rays might be described by their wavelengths, nor did he use spectrally resolving apparatus such as prisms or diffraction gratings. His work was quantitative within these constraints. He made his measurements in a room temperature environment, and quickly so as to catch his bodies in a condition near the thermal equilibrium in which they had been prepared by heating to equilibrium with boiling water. His measurements confirmed that substances that emit and absorb selectively respect the principle of selective equality of emission and absorption at thermal equilibrium. Stewart offered a theoretical proof that this should be  the case separately for every selected quality of thermal radiation, but his mathematics was not rigorously valid. He made no mention of thermodynamics in this paper, though he did refer to conservation of "vis viva". He proposed that his measurements implied that radiation was both absorbed and emitted by particles of matter throughout depths of the media in which it propagated. He applied the Helmholtz reciprocity principle to account for the material interface processes as distinct from the processes in the interior material. He did not postulate unrealizable perfectly black surfaces. He concluded that his experiments showed that in a  cavity in thermal equilibrium, the heat radiated from any part of the interior bounding surface, no matter of what material it might be composed, was the same as would have been emitted from a surface of the same shape and position that would have been composed of lamp-black. He did not state explicitly that the lamp-black-coated bodies that he used as reference must have had a unique common spectral emittance function that depended on temperature in a unique way. Gustav Kirchhoff. In 1859, not knowing of Stewart's work, Gustav Robert Kirchhoff reported the coincidence of the  wavelengths of spectrally resolved lines of absorption and of emission of visible light. Importantly for thermal physics, he also observed that bright lines or dark lines were apparent depending on the temperature difference between emitter and absorber. Kirchhoff then went on to consider some bodies that emit and absorb heat radiation, in an opaque enclosure or cavity, in equilibrium at temperature . Here is used a notation different from Kirchhoff's. Here, the emitting power denotes a dimensioned quantity, the total radiation emitted by a body labeled by index at temperature . The total absorption ratio of that body is dimensionless, the  ratio of absorbed to incident radiation in the cavity at temperature . (In contrast with Balfour Stewart's, Kirchhoff's definition of his absorption ratio did not refer in particular to a lamp-black surface as the source of the incident radiation.) Thus the ratio of emitting power to absorptivity is a dimensioned quantity, with the dimensions of emitting power, because is dimensionless. Also here the wavelength-specific emitting power of the body at temperature is denoted by and the wavelength-specific absorption ratio by . Again, the ratio of emitting power to absorptivity is a dimensioned quantity, with the dimensions of  emitting power. In a second report made in 1859, Kirchhoff announced a new general principle or law for which he offered a theoretical and mathematical proof, though he did not offer quantitative measurements of radiation powers. His theoretical proof was and still is considered by some writers to be invalid. His principle, however, has endured: it was that for heat rays of the same wavelength, in equilibrium at a given temperature, the wavelength-specific ratio of emitting power to absorptivity has one and the same common value for all bodies that emit and absorb at that wavelength. In symbols, the  law stated that the wavelength-specific ratio has one and the same value for all bodies, that is for all values of index . In this report there was no mention of black bodies. In 1860, still not knowing of Stewart's measurements for selected qualities of radiation, Kirchhoff pointed out that it was long established experimentally that for total heat radiation, of unselected quality, emitted and absorbed by a body in equilibrium, the dimensioned total radiation ratio , has one and the same value common to all bodies, that is, for every value of the material index . Again without measurements of  radiative powers or other new experimental data, Kirchhoff then offered a fresh theoretical proof of his new principle of the universality of the value of the wavelength-specific ratio at thermal equilibrium. His fresh theoretical proof was and still is considered by some writers to be invalid. But more importantly, it relied on a new theoretical postulate of "perfectly black bodies," which is the reason why one speaks of Kirchhoff's law. Such black bodies showed complete absorption in their infinitely thin most superficial surface. They correspond to Balfour Stewart's reference bodies, with internal radiation, coated with lamp-black . They were not the more realistic perfectly black bodies later considered by Planck. Planck's black bodies radiated and absorbed only by the material in their interiors; their interfaces with contiguous media were only mathematical surfaces, capable neither of absorption nor emission, but only of reflecting and transmitting with refraction. Kirchhoff's proof considered an arbitrary non-ideal body labeled as well as various perfect black bodies labeled . It required that the bodies be kept in a cavity in thermal equilibrium at temperature . His proof intended to show that the ratio was independent of the nature of the non-ideal  body, however partly transparent or partly reflective it was. His proof first argued that for wavelength and at temperature , at thermal equilibrium, all perfectly black bodies of the same size and shape have the one and the same common value of emissive power , with the dimensions of power. His proof noted that the dimensionless wavelength-specific absorptivity of a perfectly black body is by definition exactly 1. Then for a perfectly black body, the wavelength-specific ratio of emissive power to absorptivity is again just , with the dimensions of power. Kirchhoff considered, successively, thermal equilibrium with the arbitrary non-ideal  body, and with a perfectly black body of the same size and shape, in place in his cavity in equilibrium at temperature . He argued that the flows of heat radiation must be the same in each case. Thus he argued that at thermal equilibrium the ratio was equal to , which may now be denoted , a continuous function, dependent only on at fixed temperature , and an increasing function of at fixed wavelength , at low temperatures vanishing for visible but not for longer wavelengths, with positive values for visible wavelengths at higher temperatures, which does not depend on the nature of the  arbitrary non-ideal body. (Geometrical factors, taken into detailed account by Kirchhoff, have been ignored in the foregoing.) Thus Kirchhoff's law of thermal radiation can be stated: "For any material at all, radiating and absorbing in thermodynamic equilibrium at any given temperature , for every wavelength , the ratio of emissive power to absorptivity has one universal value, which is characteristic of a perfect black body, and is an emissive power which we here represent by ." (For our notation , Kirchhoff's original notation was simply .) Kirchhoff announced that the determination of the function was a problem of the highest importance, though  he recognized that there would be experimental difficulties to be overcome. He supposed that like other functions that do not depend on the properties of individual bodies, it would be a simple function. Occasionally by historians that function has been called "Kirchhoff's (emission, universal) function," though its precise mathematical form would not be known for another forty years, till it was discovered by Planck in 1900. The theoretical proof for Kirchhoff's universality principle was worked on and debated by various physicists over the same time, and later. Kirchhoff stated later in 1860 that his theoretical proof was better  than Balfour Stewart's, and in some respects it was so. Kirchhoff's 1860 paper did not mention the second law of thermodynamics, and of course did not mention the concept of entropy which had not at that time been established. In a more considered account in a book in 1862, Kirchhoff mentioned the connection of his law with Carnot's principle, which is a form of the second law. According to Helge Kragh, "Quantum theory owes its origin to the study of thermal radiation, in particular to the "black-body" radiation that Robert Kirchhoff had first defined in 1859–1860 ." Doppler effect. The relativistic Doppler effect causes a shift in the frequency "f" of light originating from a source that is moving in relation to the observer, so that the wave is observed to have frequency "f"': where "v" is the velocity of the source in the observer's rest frame, "θ" is the angle between the velocity vector and the observer-source direction measured in the reference frame of the source, and "c" is the speed of light. This can be simplified for the special cases of objects moving directly towards ("θ" = π) or away ("θ" = 0 ) from the observer, and for speeds much less than "c". Through Planck's law the temperature spectrum of a black body is proportionally related to the frequency of light and one may substitute the temperature ("T") for the frequency in this equation. For the case of a source moving directly towards or away from the observer, this reduces to Here "v" > 0 indicates a receding source, and "v" < 0 indicates an approaching source. This is an important effect in astronomy, where the velocities of stars and galaxies can reach significant fractions of "c". An example is found in  the cosmic microwave background radiation, which exhibits a dipole anisotropy from the Earth's motion relative to this black-body radiation field. Black-body radiation Black-body radiation is the thermal electromagnetic radiation within or surrounding a body in thermodynamic equilibrium with its environment, emitted by a black body (an idealized opaque, non-reflective body). It has a specific, continuous, spectrum of wavelengths, inversely related to intensity that depend only on the body's temperature, which is assumed for the sake of calculations and theory to be uniform and constant. A perfectly insulated enclosure that is in thermal equilibrium internally