General relativity reduces to Newtonian gravity in weak-field, slow-motion approximation.The Newtonian limit is the regime in which general relativity, Einstein's theory of gravity, simplifies to Isaac Newton's classical law of universal gravitation. This happens when gravitational fields are weak (much weaker than the energy density of the masses involved) and objects move slowly compared to the speed of light. In this limit, the curved spacetime of relativity reduces to flat space with a small perturbation, and the equations of motion become the familiar Newtonian ones.
The concept was implicit in Einstein's 1915 development of general relativity, as he explicitly showed that his theory reproduced Newtonian gravity in the appropriate limit. The formal mathematical treatment of the post-Newtonian expansion, which systematically extends this limit, was developed later by Einstein, Infeld, and Hoffmann in 1938.
In general relativity, gravity is described by the curvature of spacetime, encoded in the metric tensor. In the Newtonian limit, the metric is nearly flat, differing only slightly from the Minkowski metric of special relativity. The time-time component of this metric perturbation is proportional to the Newtonian gravitational potential. When you plug this into the geodesic equation (the path a free-falling object follows), you recover Newton's second law with the gravitational force. Similarly, the Einstein field equations reduce to Poisson's equation for the gravitational potential.
It is used to compute gravitational effects in everyday and astronomical contexts, such as satellite orbits, planetary motion, and GPS corrections, where relativistic corrections are small but measurable.
The Newtonian limit also explains why we don't notice gravitational time dilation in daily life: the effect is proportional to the gravitational potential, which on Earth's surface is tiny compared to the speed of light squared.












