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.