In
relativity theory,
proper acceleration is the physical
acceleration (i.e., measurable acceleration as by an
accelerometer) experienced by an object. It is thus acceleration relative to a
free-fall, or inertial, observer who is momentarily at rest relative to the object being measured. Gravitation therefore does not cause proper acceleration, since gravity acts upon the inertial observer that any proper acceleration must depart from (accelerate from). A corollary is that all inertial observers always have a proper acceleration of zero.