The Equivalence Principle
Acceleration as Gravity & Curved Spacetime
Earth surface g
9.81 m/s²
Inertial mass
m_i
Gravitational
m_g = m_i
WEP precision
< 10⁻¹⁵
GR foundation
Strong EP
Free-fall
Locally inertial
Weak EP: all objects fall at the same rate in a gravitational field, regardless of their composition or mass. Inertial mass equals gravitational mass — exactly.
Einstein EP: a uniform gravitational field is locally indistinguishable from a uniformly accelerating frame. No experiment performed in a sealed lift can tell which one you are in.
Strong EP: the result extends to every law of physics — including the behaviour of light, clocks, and other gravitational systems. This is the rock on which general relativity is built.
ISS astronauts
Free-fall ≡ inertialCrew on the International Space Station feel weightless not because gravity is absent — it's still ~89% of surface strength up there — but because they and the station are in identical free-fall. Locally, free-fall is indistinguishable from deep space.
MICROSCOPE satellite (2017)
≤ 10⁻¹⁵A space-based test dropping titanium and platinum test masses inside a satellite confirmed that inertial mass equals gravitational mass to 1 part in 10¹⁵ — by far the most stringent verification of the weak equivalence principle.
Pound–Rebka (1960)
Δf/f ≈ 2.5 × 10⁻¹⁵Photons climbing a 22.5 m tower at Harvard lost energy by exactly the predicted amount. The equivalence principle implies clocks higher in a gravity well tick faster — the same gravitational time dilation that GPS satellites must correct for daily.
Einstein's happiest thought
1907 → GR (1915)In 1907, Einstein realised that a person in free-fall feels no gravity. That single insight — equivalence — became the seed of general relativity. Gravity is not a force pulling you down; it is the geometry of spacetime, and free-fall is the natural straight line through it.
