The simplest black hole solution, with no charge or rotation, described by Karl Schwarzschild.A Schwarzschild black hole is the simplest type of black hole, characterized by having mass but no electric charge and no angular momentum (rotation). It is described by a solution to Einstein's field equations of general relativity, derived by Karl Schwarzschild in 1916. This solution describes a spherically symmetric, non-rotating black hole with a single event horizon.
Karl Schwarzschild derived this solution in 1916, just months after Einstein published general relativity, while serving on the German front in World War I. It was the first exact solution to Einstein's field equations.
The Schwarzschild solution predicts that if a mass is compressed within a critical radius (the Schwarzschild radius), it forms a black hole. The event horizon is the boundary beyond which nothing, not even light, can escape. The geometry of spacetime around a Schwarzschild black hole is static and spherically symmetric, with a singularity at the center where curvature becomes infinite.
Schwarzschild black holes are used as theoretical models to study gravitational lensing, accretion disk physics, and the behavior of matter under extreme gravity. They also serve as a baseline for testing more complex black hole solutions.
The Schwarzschild radius of the Sun is about 3 kilometers, meaning if the Sun were compressed to that size, it would become a black hole.









