The geodesic equation describes the path a free-falling object follows in curved spacetime due to gravity.The geodesic equation is a central element of Einstein's general theory of relativity. It generalizes Newton's law of inertia to curved spacetime. A massive body bends the spacetime continuum, and a test particle moves along a line that minimizes proper time (the time measured by a clock moving with the particle). Geometrically, this is described through Christoffel symbols — quantities characterizing curvature. The equation looks like d²x^μ/dτ² + Γ^μ_{νρ} (dx^ν/dτ)(dx^ρ/dτ) = 0, where the first term is Newtonian acceleration, and the second is the curvature correction.
The concept of a geodesic line goes back to the work of Gauss and Riemann in differential geometry. In 1915, Albert Einstein completed the general theory of relativity, in which the motion of free particles along geodesics became a direct consequence of the field equations. The mathematical form with symmetric connection was developed by Marcel Grossmann and Elwin Bruno Christoffel (Christoffel symbols). Later, relativists, notably John Archibald Wheeler, developed the geometric interpretation of gravity as curvature of spacetime.
Used in astrophysics to calculate the trajectories of bodies in strong gravitational fields (black holes, neutron stars) and in cosmology to model the propagation of light in an expanding universe. Limits of applicability: classical GR, neglecting quantum effects and the object's size (test particle). In the weak-field, low-velocity limit, it reduces to Newton's equation of motion.
The geodesic equation is used to calculate the orbits of GPS satellites and the trajectories of space probes taking gravity into account.
Light, having no mass, also moves along geodesics, but null ones, which define the trajectories of massless particles. This leads to gravitational lensing — the distortion of images of distant galaxies.








