In 1913, Niels Bohr proposed a model to accurately describe the hydrogen atom's structure and its spectral lines. According to Bohr's postulates, electrons orbit the nucleus in fixed paths called orbits or stationary states, each with a quantized energy level. An electron can only occupy certain allowed orbits, and energy is absorbed or emitted when it moves between these states. Bohr derived the expression for the electron's angular momentum in these orbits, revealing that it takes on discrete values—integral multiples of h/2π. This model successfully rationalized the hydrogen spectrum but failed for multi-electron systems, highlighting its limitations. Despite drawbacks, Bohr's approach set the foundation for later developments in quantum mechanics.