Stefan-Boltzmann law

Also called Stefan's law

The Stefan-Boltzmann law gives the power a blackbody radiates as P = A sigma T^4: emitting surface area times the Stefan-Boltzmann constant times absolute temperature raised to the fourth power, with T in kelvin.

Required content in AP Physics 2, not an extra. Essential knowledge 15.4.A.3.iii states that the rate at which energy is emitted (power) by a blackbody is proportional to the surface area of the body and to the temperature of the body raised to the fourth power, and it names the Stefan-Boltzmann law.

P=AσT4P = A \sigma T^4

Printed in the Modern Physics group of the AP Physics 2 sheet, with σ=5.67×108 W/(m2K4)\sigma = 5.67 \times 10^{-8}\ \mathrm{W/(m^2 \cdot K^4)} in the constants table.

What each symbol carries. PP is radiated power in watts, AA the emitting surface area in square metres, TT the absolute temperature in kelvin. Convert a Celsius reading first: the law is written for absolute temperature, and a ratio of Celsius readings is not a ratio of temperatures.

The fourth power is where the marks are. Suggested skill 2.C for Topic 15.4 is comparing a quantity between two scenarios, and this equation rewards a ratio more than a calculation. Double TT and the emitted power rises by 24=162^4 = 16. Triple it and the rise is 34=813^4 = 81. Area scales only linearly, so a small hot filament outradiates a large warm wall.

Where the law lives. It sits in Unit 15 with the blackbody model, not in the Unit 9 heat transfer topic where thermal radiation is first named. Reach for it when a question asks for emitted power, not when it asks you to name a transfer pathway. Wien's law locates the peak of the same spectrum; this one totals it.

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