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Thus, the Wien law explains the shift of the peak to shorter wavelengths as the temperature increases. Notice that the variation of the peak of intensity with temperature is much less rapid than that of the intensity itself. The intensity varies as the fourth power of the temperature, but the peak position varies only inversely with T. For example, if T is doubled, the peak wavelength is decreased by a factor of two but the peak height is increased by a factor of sixteen.
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For convenience in plotting, these distributions have been normalized to unity at the respective peaks; by the Stefan-Boltzmann law, the area under the peak for the hot star Spica is in reality 2094 times the area under the peak for the cool star Antares.
| Some Blackbody Temperatures | |||
|---|---|---|---|
| Radio | > 10 | < 10-5 | < 0.03 |
| Microwave | 10 - 0.01 | 10-5 - 0.01 | 0.03 - 30 |
| Infrared | 0.01 - 7 x 10-5 | 0.01 - 2 | 30 - 4100 |
| Visible | 7 x 10-5 - 4 x 10-5 | 2 - 3 | 4100 - 7300 |
| Ultraviolet | 4 x 10-5 - 10-7 | 3 - 103 | 7300 - 3 x 106 |
| X-Rays | 10-7 - 10-9 | 103 - 105 | 3 x 106 - 3 x 108 |
| Gamma Rays | < 10-9 | > 105 | > 3 x 108 |
(The notation "eV" stands for electron-Volt, a common unit of energy.)
As noted in the right panel, the peak temperatures quoted in this table are valid only
if the spectrum is a thermal (blackbody) spectrum. The behavior of a nonthermal spectrum
is not governed by the Wien law.