
Gravity as described by general relativity, without quantum effects.Classical gravity refers to the description of gravitational phenomena using general relativity, without incorporating quantum mechanics. It encompasses the curvature of spacetime caused by mass and energy, as described by Einstein's field equations. Classical gravity successfully explains phenomena from planetary orbits to black holes, gravitational lensing, and the expansion of the universe. However, it breaks down in extreme conditions such as the Big Bang singularity or the interior of black holes, where quantum effects become significant.
General relativity was developed by Albert Einstein in 1915, building on the equivalence principle and the mathematics of differential geometry. It replaced Newton's law of universal gravitation as a more accurate description of gravity, and has been confirmed by numerous experiments and observations.
In classical gravity, spacetime is a dynamical entity that curves in response to the presence of matter and energy. Objects move along geodesics, which are the straightest possible paths in curved spacetime. The Einstein field equations relate the curvature of spacetime to the stress-energy tensor, providing a deterministic evolution of the geometry. This framework is purely classical, meaning it does not account for quantum fluctuations or the discrete nature of particles.
Classical gravity is used in GPS satellite navigation, where relativistic corrections are essential for accurate positioning. It also underpins astrophysical models of stellar evolution, black hole accretion, and gravitational wave astronomy.
Classical gravity predicts that time runs slower in stronger gravitational fields, an effect that must be corrected for in GPS satellites to maintain accuracy.















