While Newton's equations are incredibly accurate for most practical purposes (including sending rockets to the moon), they break down when dealing with extremely massive objects or speeds approaching the speed of light.
General Relativity
In 1915, Albert Einstein published his General Theory of Relativity, fundamentally redefining gravity. According to Einstein, gravity is not a "force" that reaches across space, but rather a consequence of the curvature of spacetime caused by the uneven distribution of mass and energy.
Imagine spacetime as a trampoline. If you place a heavy bowling ball in the center, it creates a dip. If you roll a marble across the trampoline, its path will curve around the bowling ball. The marble isn't being "pulled" by a mysterious force; it is simply following the straightest possible path (a geodesic) through a curved space.
This is governed by the Einstein Field Equations:
$$
R_{\mu\nu} - \frac{1}{2}R g_{\mu\nu} + \Lambda g_{\mu\nu} = \frac{8\pi G}{c^4} T_{\mu\nu}
$$
Where:
- Rμν and R describe the curvature of spacetime.
- gμν is the metric tensor.
- Λ is the cosmological constant.
- Tμν is the stress-energy tensor (representing the distribution of mass and energy).
In short, John Archibald Wheeler perfectly summarized General Relativity: "Spacetime tells matter how to move; matter tells spacetime how to curve."