Relativityundergraduate

Einstein Equivalence Principle

Also known as: Equivalence principle · EEP · Weak/strong equivalence

Inside a sealed elevator you cannot tell gravity from acceleration: a falling lab and a coasting rocket give identical physics. Because gravitational and inertial mass are the same number, everything falls at the same rate — so 'gravity' is locally just the geometry of an accelerating frame.

mi=mg    glocalam_i = m_g \;\Rightarrow\; \vec{g}_{\text{local}} \equiv -\vec{a}
Live simulation
warming up the physics…

Side-by-side: a box accelerating in empty space vs a box at rest on a planet. A released ball traces the identical parabola in both, showing the two scenes are physically indistinguishable.

Equivalent forms

weak eep
mix¨=mgg,mi=mgm_i \ddot{\vec{x}} = m_g \vec{g},\quad m_i = m_g
redshift form
Δνν=ghc2\frac{\Delta \nu}{\nu} = \frac{g h}{c^2}
The deepest free lunch in physics: equating two a-priori unrelated masses turns gravity from a force into the curvature of spacetime.