Although stars are not perfect blackbodies, they can be approximated as such, allowing us to calculate their surface temperature via the Stefan-Boltzmann Law:
where | luminosity of the star | ||
star’s radius | |||
Stefan-Boltzmann constant | |||
effective temperature |
The surface temperature, calculated by assuming a perfect blackbody radiating the same amount of energy per unit area as the star, is known as the effective temperature of the star.
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