Theory of relativity
The equivalence principle
Compare the motion of a free body inside an accelerating frame with motion in a uniform gravitational field, and verify that locally the two descriptions are indistinguishable — the equivalence principle at the heart of general relativity.
Equipment
- 3D canvas: accelerating elevator plus curved-grid view near a mass
- Slider “accelerating frame” (frame acceleration)
- Slider “Tốc độ thời gian” (animation speed) and “Tạm dừng” button
Procedure
Release a body in the accelerating frame
Set a moderate acceleration on the “accelerating frame” slider and watch the free body's path in the elevator. In the accelerated frame it appears to fall with acceleration , exactly as if a uniform gravitational field pulled it — no local experiment distinguishes the two.
Match acceleration to gravity
Raise and lower the acceleration and compare with the warped-grid view near the mass. Find the slider setting where the apparent fall in the elevator reproduces free fall in the gravitational field, confirming .
Probe the local limit
Ask what would spoil the equivalence: over a large region, tidal effects — the variation of g from place to place — betray real gravity. Pause the model and explain why the equivalence principle holds only in a sufficiently small neighborhood and is the seed of curved-spacetime gravity.