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  1. Electromagnetic waves emitted by a blackbody are called blackbody radiation. Figure \(\PageIndex{2}\): The intensity of blackbody radiation versus the wavelength of the emitted radiation. Each curve corresponds to a different blackbody temperature, starting with a low temperature (the lowest curve) to a high temperature (the highest curve).

  2. m. ‪Spectral Power Density (MW/m²/µm)‬ ‪Wavelength (µm)‬ ‪1 µm = 1000 nm‬ 0 3 ‪100‬ ‪X-Ray‬ ‪Ultraviolet‬ ‪Visible‬ ‪Infrared‬ 0.500 ‪84.46‬ ‪Graph Values‬ ‪Labels‬ ‪Intensity‬ 5800 ‪K‬?? ‪Sirius A‬ ‪Sun‬ ‪Light Bulb‬ ‪Earth‬ ‪Blackbody‬ ‪Temperature‬ 5800 ‪K ...

  3. 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).

  4. The spectrum of blackbody radiation has a typical bell shape and the emitted energy (integral of the curve) is proportional to the forth power of the absolute temperature (T 4): hotter bodies radiate a lot more. The following plot shows the spectrum for temperatures from 273 K (0 °C) to 453 K (180 °C) in 20 °C steps.

  5. The intensity I (λ, T) I (λ, T) of blackbody radiation depends on the wavelength λ λ of the emitted radiation and on the temperature T of the blackbody .

  6. All material objects with a temperature above absolute zero emit electromagnetic radiation. The radiation represents a conversion of a body’s thermal energy into electromagnetic energy, and is therefore called thermal radiation. Conversely all matter absorbs electromagnetic radiation to some degree.

  7. Function: Plank Blackbody Emission¶ Total Exitance = M = εσT^4 and the Peak = 2897/T (Watts) Where T is the absolute temperature, ε is the emissivity (= 1 for blackbody), and σ = 5.67036×10−8 W/m^2⋅K^4 is the Stefan–Boltzmann constant.

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