Mission clocks: the maths
The weak-field approximation of general relativity for clocks in circular orbit (the Moon base adds the Moon's own gravity). Computed live.
Equations
- Δf/f ≈ GM/c² · (1/R − 1/r) − GM/(2rc²)
- Rate against a ground clock: gravity (higher is faster) minus orbital speed (faster is slower); × 86,400 × 10⁶ for µs per day.
- Δt = Δf/f × days
- What the clock gains or loses over the mission.
Constants
| GM | 3.986004418 × 10¹⁴ m³/s² | Earth (IERS) |
| R | 6,371 km | Earth's mean radius |
| c | 299,792,458 m/s | exact |
Worked examples ✓ checked on every change
| ISS (408 km): rate per day | -24.6 µs/day | the formula above: speed wins |
| GPS (20,200 km): rate per day | +38.6 µs/day | Ashby (2003) |
| Six months on the ISS: total | -4.50 ms | about 4.5 thousandths of a second younger |
What's simplified
- Circular orbits; Earth doesn't rotate in the model, so the ground clock's own small motion is ignored.
- The Moon base uses the Moon's surface gravity plus its orbit around Earth.
Where it breaks
Near very strong gravity (neutron stars, black holes), where the weak-field formula stops being accurate.
Sources: N. Ashby, Living Rev. Relativ. 6, 1 (2003); IERS Conventions (2010).