tidal forces
Tidal forces are the stretching and squeezing that arise because gravity is not exactly the same everywhere across an extended object. The near side of a body is pulled a little harder than the far side, and the sides are pulled slightly inward toward the center, so the object gets stretched along the line toward the source and pinched across it. The ocean tides are the everyday example: the Moon tugs the near ocean more strongly than the solid Earth, and the Earth more strongly than the far ocean, raising a bulge of water on both sides.
The deep significance is that tidal forces are the part of gravity you cannot make disappear. The equivalence principle says that by free-falling, you can erase the uniform pull of gravity inside a small box — but only inside a small box. Stretch the box larger, and the pull at the top differs from the pull at the bottom; that difference survives no matter what frame you choose, because it is a real, frame-independent fact about the field. An astronaut floating freely feels weightless, but two balls released far apart slowly drift — together horizontally, apart vertically — revealing the tidal pattern that no acceleration can mimic away.
This is exactly why tidal forces are the true signature of spacetime curvature. In general relativity, nearby free-falling paths are geodesics, and tidal effects are these geodesics converging or spreading apart — geometry, not a force. Where the curvature is gentle, tides are mild; where it is extreme, they are lethal. Fall feet-first toward a stellar black hole and the difference in pull between your feet and head would stretch you into a thin stream, a fate vividly nicknamed 'spaghettification.'
The tidal stretch across a small height Δr grows as 1/r³ — gentle far away, ferocious close to a compact mass.
Uniform gravity can always be transformed away by free-falling; tidal differences cannot. That irreducible residue is precisely what 'spacetime curvature' means — gravity proper, not an accelerated point of view.