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How GPS Positioning Works

The Global Positioning System consists of 31 active satellites orbiting at approximately 20,200 km altitude, in six orbital planes. Each satellite continuously broadcasts a signal containing:

  1. Its precise location in space (ephemeris data)
  2. The exact time of transmission (from atomic clocks accurate to ~20 ns)

Your receiver picks up signals from ≥4 satellites simultaneously. The time difference between transmission and reception, multiplied by the speed of light (c = 3 × 10⁸ m/s), gives the distance (range) to each satellite:

range = c × Δt

With four ranges, four simultaneous equations can be solved for three position coordinates (x, y, z) and the receiver's clock error. This is trilateration — not triangulation.

The critical dependency: the system only works if every satellite's clock is perfectly synchronised with every other satellite and with the ground. An error of just 1 nanosecond = 30 cm position error. The required timing precision is extraordinary — and this is exactly where relativity becomes essential.

Special Relativity — Time Dilation from Velocity

Einstein's 1905 special relativity contains the result that moving clocks tick slower than stationary ones. The time dilation formula:

Δtmoving = Δtrest × √(1 − v²/c²)

GPS satellites orbit at v ≈ 3.87 km/s (14,000 km/h). Relative to a stationary ground receiver:

1 − v²/c² = 1 − (3870)²/(3×10⁸)² = 1 − 1.66 × 10⁻¹⁰ ≈ 0.9999998

The fractional rate difference: Δf/f = −v²/2c² = −8.3 × 10⁻¹¹

Over one day (86,400 s): ΔtSR = 8.3 × 10⁻¹¹ × 86,400 s ≈ −7.2 microseconds per day

Special relativity makes the satellite clocks tick slower than ground clocks — they would lose 7.2 μs/day.

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General Relativity — Gravitational Time Dilation

Einstein's 1915 general relativity introduces a second, independent effect: clocks at higher gravitational potential tick faster. The gravitational time dilation formula:

Δthigh / Δtlow = √(1 − 2GM/rc²) / √(1 − 2GM/R_E c²) ≈ 1 + gh/c²

where h is the altitude, g ≈ 9.8 m/s² (near Earth's surface), and c = 3 × 10⁸ m/s. For a GPS satellite at h = 20,200 km:

ΔtGR/day = (gh/c²) × 86,400 s = (9.8 × 20,200,000) / (9 × 10¹⁶) × 86,400 ≈ +45.9 μs/day

General relativity makes the satellite clocks tick faster than ground clocks — they would gain 45.9 μs/day.

The Exact Numbers

The two effects act in opposite directions:

EffectSourceClock change per dayDirection
Special RelativisticOrbital velocity (3.87 km/s)−7.2 μsSlower (time dilation)
General RelativisticAltitude (+20,200 km)+45.9 μsFaster (gravitational)
Net effectCombined+38.7 μs/dayFaster overall

If uncorrected, GPS satellite clocks would gain approximately 38.7 microseconds per day relative to ground clocks. Since 1 μs = 300 m of positional error, 38.7 μs → ~11.6 km position error per day — accumulating constantly.

How the Correction Is Applied

The GPS system applies relativistic corrections in two ways:

  1. Pre-launch clock rate offset: Satellite atomic clocks are deliberately set to tick at a rate slightly lower than nominal before launch — specifically at f = f₀ × (1 − 4.465 × 10⁻¹⁰) = 10.229 999 995 43 MHz instead of 10.23 MHz. This pre-accounts for the net +38.7 μs/day GR/SR combined drift, making the satellite clock appear to tick at exactly the standard rate as observed from the ground.
  2. Shapiro delay corrections: The navigation message also applies additional real-time corrections for the Sagnac effect (Earth's rotation), orbital eccentricity (satellite speed and altitude vary slightly), and tropospheric/ionospheric propagation delays.

What Happens Without the Correction

This is not hypothetical — the engineers who designed GPS debated whether relativistic effects would be large enough to matter. Some argued relativity could be ignored. The decision was ultimately made to apply the corrections before launch.

If the corrections were turned off today:

  • After 1 hour: position error ≈ ~500 m
  • After 1 day: position error ≈ ~11.6 km
  • After 1 week: position error ≈ ~80 km

Aviation navigation, financial transaction timestamping, mobile network synchronisation, and precision agriculture all depend on GPS timing — they would all fail progressively.

Other Relativistic Effects in GPS

The Sagnac Effect

Earth's rotation means the ground receiver moves during the time a GPS signal travels from satellite to receiver. The signal path length changes as the receiver moves. This introduces an apparent timing error proportional to the area swept by the signal triangle and Earth's angular velocity Ω:

ΔtSagnac = 2Ω·A / c²

For GPS signals, the Sagnac correction is up to ~200 ns (60 m equivalent) and is applied continuously in real time.

Orbital Eccentricity (Relativistic Doppler)

GPS satellite orbits are not perfectly circular — they have a small eccentricity (e ≈ 0.01). As the satellite moves faster at periapsis (closest approach) and slower at apoapsis, both SR and GR effects vary continuously. This introduces a periodic correction that must be computed from the broadcast ephemeris data.

Shapiro Delay

Light (and radio signals) travel slightly more slowly through warped spacetime near a massive body. GPS signals passing close to Earth's surface experience a Shapiro delay of ~10 ns per pass — small but measurable, applied as a correction for high-precision applications.

💡 The Ultimate Test of Relativity in Everyday Life

GPS represents the most widespread practical application of both special and general relativity simultaneously. Over 4 billion people use GPS daily. Every time you navigate with your phone, both of Einstein's relativity theories are at work — correcting your position to within metres.

📚 Recommended Reading

🛰
Relativity: The Special and General Theory (Einstein)
Albert Einstein
Original — readable
View on Amazon
🌎
Was Einstein Right? (Will)
Clifford Will
Popular science
View on Amazon

ℹ Amazon Associate.

Frequently Asked Questions

Does GPS really use relativity?

Yes. Both special relativistic time dilation (satellite velocity) and general relativistic gravitational time dilation (satellite altitude) produce measurable, significant timing errors. Without corrections, GPS would fail within hours. The correction has been applied since the first operational GPS satellite in 1978.

What is the relativistic correction for GPS?

SR effect: −7.2 μs/day (clocks slow due to speed). GR effect: +45.9 μs/day (clocks fast due to altitude). Net: +38.7 μs/day corrected by pre-slowing satellite clocks by 4.465 × 10⁻¹⁰ Hz before launch.

Does general relativity really affect time in daily life?

Yes. GPS is the most prominent example. Additionally, time runs measurably faster at high altitude (mountain tops) than at sea level — demonstrated by atomic clock comparisons between ground and aircraft (Hafele-Keating experiment, 1971), and by precise measurements between clocks at different heights (confirmed at just 33 cm height difference by optical lattice clocks, NIST 2010).

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