Einstein (I)
•Einstein (1907): “hypothesis of complete physical equivalence”
In a freely falling system all masses fall equally fast, hence gravitational acceleration has no local dynamical effects
Weak Equivalence Principle (WEP)
An observer inside Einstein elevator will not be able to tell, before hitting the ground, whether he is moving with an acceleration g in empty space, far away from all masses, or else he is falling in the vicinity (height of fall<<Earth radius) of a body (the Earth) whose local gravitational acceleration is also g (and in the same direction).