You now have the pieces: sunlight arrives, albedo decides how much is absorbed, and every surface glows by the Stefan–Boltzmann law. Put them together and you can predict the temperature of a planet from two numbers, using a fourth root.
Key idea
Why it works
Worked example: Earth with no greenhouse effect
- Average sunlight per square meter: $1361 \div 4 \approx 340$ W/m².
- Absorbed: $(1 - 0.30) \times 340 \approx 238$ W/m².
- Set $\sigma T^4 = 238$: $T^4 = 238 \div (5.67 \times 10^{-8}) \approx 4.20 \times 10^{9}$.
- $T = (4.20 \times 10^{9})^{1/4} \approx 255$ K, or about −18 °C.
Answer: About 255 K (−18 °C)
Worked example: A planet four times as far
- Sunlight spreads as the square of distance, so $S$ is $4^2 = 16$ times smaller.
- $T_e$ goes as $S^{1/4}$, so it changes by $(1/16)^{1/4} = 1/2$.
- $T_e \approx 255 \div 2 \approx 127$ K. No calculator needed.
Answer: About 127 K
Worked example: A snowball Earth
- Absorbed: $(1 - 0.60) \times 340 = 136$ W/m².
- $T^4 = 136 \div (5.67 \times 10^{-8}) \approx 2.40 \times 10^{9}$, so $T \approx 221$ K (−52 °C).
- A whiter planet absorbs less sunlight and settles much colder.
Answer: About 221 K
Common mistake
Earth's real average surface temperature is about 15 °C (288 K), some 33 °C warmer than this balance temperature. The difference is the greenhouse effect, the subject of the next lesson. Satellites confirm the outgoing side: Earth sends about 240 W/m² of infrared to space, just as this calculation predicts.