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Black radiation from

Blackbody Radiation Engineering calculations of thermal radiation from surfaces are best keyed to the radiation characteristics of the blackbody, or ideal radiator. The characteristic properties of a blackbody are that it absorbs all the radiation incident on its surface and that the quality and intensity of the radiation it emits are completely determined by its temperature. The total radiative fliix throughout a hemisphere from a black surface of area A and absolute temperature T is given by the Stefan-Boltzmann law ... [Pg.570]

The radiation from a blackbody is conhnuous over the electromagnetic spectrum. The use of the term black in blackbody, which implies a particular color, is quite misleading, as a number of nonblack maferials approach blackbodies in behavior. The sun behaves almost like a blackbody snow radiates in the infrared nearly as a blackbody. At some wavelengths, water... [Pg.245]

The radiation from a black body is proportional to the fourth power of the adiabatic flame temperature, according to the Stefan-Boltzmann s law ... [Pg.167]

The heat flux radiated from a real surface is less than that from an ideal black body surface at the same temperature. The ratio of real to black body flux is the normal total emissivity. Emissivity, like thermal conductivity, is a property which must be determined experimentally. [Pg.346]

Electrically-heated carbide elements, JO mm in diameter and 0.5 m long, radiating essentially as black bodies, are to be used in the construction of a heater in which thermal radiation from the surroundings is negligible. If the surface temperature of the carbide is limited to 1750 K, how many elements are required to provide a radiated thermal output of 500 kW7... [Pg.441]

Figure 8.30. Theoretical energy flux for radiation from the sun as a black body at 5,800 K. The spectrum reaching the surface of the earth is modified through absorption in the infrared region by H2O and CO2 and in the... Figure 8.30. Theoretical energy flux for radiation from the sun as a black body at 5,800 K. The spectrum reaching the surface of the earth is modified through absorption in the infrared region by H2O and CO2 and in the...
Let a small black body of area S and at temperature T2, completely enveloped by a hotter black body at temperature Tlr be considered. In this case, the net amount of heat transferred from the hotter to the colder body equals the algebraic sum of the radiations from the two bodies and is given by... [Pg.321]

The Stefan-Boltzmann Law and Wien s Law for black body radiation have been unified into Planck s Law for black body radiation, from which Planck s constant was first introduced. Planck s analysis of the spectral distribution of black body radiation led him to an understanding of the quantisation of energy and radiation and the role of the photon in the theory of radiation. The precise law relates the intensity of the radiation at all wavelengths with the temperature and has the form ... [Pg.18]

The black body radiation model for the continuum radiation from stars works well but it is not quite right. Careful consideration of the radiation profile shows deviations from the curves shown in Figure 2.1 due to the structure of the star itself. These deviations form the basis of a more detailed analysis including the effects of circulation within the star and will be left to others to explain we shall use black body radiation as our model for stars. [Pg.20]

Dispersing the radiation from the star into its component wavelengths reveals that the spectrum of a star is not the continuous spectrum of a black body but there are... [Pg.56]

The radiation coming from a black body is continuous in wavelength but dispersing the radiation from a star reveals absorption lines, which can be identified clearly... [Pg.86]

Radiation from AGNs, some of which can also be reprocessed by dust, but which differs from the other two sources in being powered by gravitational rather than nuclear energy and therefore not associated with nucleosynthesis. This contribution is probably minor, however, based on the abundance of massive black holes (Madau Pozzetti 2000), or on that of obscured hard X-ray sources (Brusa, Comastri Vignali 2001). [Pg.397]

C 6 m, 1000 °C 15 m, 1100°C and 30 m, 1200 °C [14], The explanation is provided by Koseki [15] (Figure 10.12), showing how Xr decreases for large-diameter fires as eddies of black soot can obscure the flame. The eddy size or soot path length increases as the fire diameter increases, causing the transmittance of the external eddies to decrease and block radiation from leaving the flame. From Table 10.2,... [Pg.315]

When a cured propellant formulation is transparent to radiation from the flame front, adjustment of the opaqueness by using carbon black can yield valuable changes in performance. [Pg.90]

The quantum concept was introduced by Max Planck in 1900 to explain the distribution of energy radiated from a black body in thermal equilibrium with the surrounding. The idea that light travels as photons was originated by Einstein in 1905. [Pg.16]

This same oxide exists in a variety of other forms, such os a fibrous mass, with the fibres radiating from a centre, in which state it is termed the red hematite or fibrous iron ore. When the ore is an amorphous mass, it is termed compact iron, ore when mixed with clay and other earthy matters, red ochre when hard, and combined with silica, jaspery ore / whon in scales of a black metallic lustra, it is known as micaceous iron ore or iron glance. [Pg.407]

Boltzmann s Law. The law of the equipartition of energy to a molecular system. Stef an-Boltzmann Law states that the total energy radiated from a black body is proportional to its absolute temp raised to the fourth power. It is expressed by E= a (T4 - T ) where E - total energy in ergs,... [Pg.222]


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Radiation from a black body

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