The Stefan–Boltzmann law describes the power radiated from a black body in terms of its temperature. The equation is:
\[
E = \sigma T^4
\]
Where:
\( E \) = emissive power (energy radiated per unit area)
\( \sigma \) = Stefan–Boltzmann constant \((5.67 \times 10^{-8} \, \text{W/m}^2\text{K}^4)\)
\( T \) = absolute temperature in Kelvin
This law is fundamental in thermal radiation theory and applies specifically to black bodies, which are idealized physical bodies that absorb all incident radiation.
Therefore, the Stefan–Boltzmann constant is used in calculating the total radiation emitted by a black body.