Earth's energy budget: the maths
A one-layer greenhouse model: Earth absorbs sunlight and radiates as a black body, with one atmospheric layer absorbing a share ε of the outgoing infrared. Computed live.
Equations
- Q = (1 − A) S₀ / 4
- Sunlight absorbed per square metre, averaged over the whole globe (a disc's worth of sunlight spread over a sphere). A is the share reflected.
- Te = (Q / σ)1/4
- The temperature Earth radiates to space at.
- Ts = Te · (2 / (2 − ε))1/4
- The surface temperature under a layer absorbing a share ε of the infrared.
Constants
| S₀ | 1361 W/m² | sunlight at Earth (Kopp & Lean 2011) |
| σ | 5.670374 × 10⁻⁸ W m⁻² K⁻⁴ | Stefan–Boltzmann, exact |
| A | 0.30 | Earth's albedo |
| ε | 0.78 | set so the surface comes out at today's 15 °C |
Worked examples ✓ checked on every change
| Earth's radiating temperature | 255.0 K | the textbook 255 K |
| Surface with no greenhouse | -18.0 °C | the textbook −18 °C |
| Surface with today's greenhouse | 15.0 °C | today's global average, about 15 °C |
What's simplified
- One layer, one temperature; no weather, oceans or feedbacks.
- ε is tuned to today's average, not calculated.
Where it breaks
For forecasts or feedbacks — ice, clouds, water vapour — which is what full climate models add. This is a teaching model, and says so.
Sources: Kopp & Lean, GRL 38 (2011); any climate textbook (e.g. Pierrehumbert, Principles of Planetary Climate, 2010).