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Chapter 11 FUNDAMENTALS OF THERMAL RADIATION

Chapter 11 FUNDAMENTALS OF THERMAL RADIATION

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<strong>Chapter</strong> <strong>11</strong> Fundamentals of Thermal RadiationRadiation Properties<strong>11</strong>-36C The emissivity is the ratio of the radiation emitted by the surface to the radiation emitted by ablackbody at the same temperature. The fraction of radiation absorbed by the surface is called theabsorptivity ,( )( T) E TE ( T)and absorbed radiationincident radiationbWhen the surface temperature is equal to the temperature of the source of radiation, the total hemisphericalemissivity of a surface at temperature T is equal to its total hemispherical absorptivity for radiationcoming from a blackbody at the same temperature ( T) ( T).GabsG<strong>11</strong>-37C The fraction of irradiation reflected by the surface is called reflectivity and the fractiontransmitted is called the transmissivity G GrefandGtr GSurfaces are assumed to reflect in a perfectly spectral or diffuse manner for simplicity. In spectral (ormirror like) reflection, the angle of reflection equals the angle of incidence of the radiation beam. In diffusereflection, radiation is reflected equally in all directions.<strong>11</strong>-38C A body whose surface properties are independent of wavelength is said to be a graybody. Theemissivity of a blackbody is one for all wavelengths, the emissivity of a graybody is between zero and one.<strong>11</strong>-39C The heating effect which is due to the non-gray characteristic of glass, clear plastic, or atmosphericgases is known as the greenhouse effect since this effect is utilized primarily in greenhouses. Thecombustion gases such as CO 2 and water vapor in the atmosphere transmit the bulk of the solar radiationbut absorb the infrared radiation emitted by the surface of the earth, acting like a heat trap. There is aconcern that the energy trapped on earth will eventually cause global warming and thus drastic changes inweather patterns.<strong>11</strong>-40C Glass has a transparent window in the wavelength range 0.3 to 3 m and it is not transparent tothe radiation which has wavelength range greater than 3 m. Therefore, because the microwaves are in therange of 10 2 to 10 5 m, the harmful microwave radiation cannot escape from the glass door.<strong>11</strong>-17

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