In quantum mechanics, the angular momentum for a hydrogen atom is described by the equation L = √(l(l+1))ħ. When L = 0, it indicates that l must also be 0, resulting in a wave function that is spherically symmetric and lacks angular dependence. This spherically symmetric condition is not exclusive to hydrogen; it also applies to other potential energy systems, such as the 3D harmonic oscillator and spherical potential wells. In these cases, energy eigenfunctions with L = 0 maintain the same spherical symmetry. Understanding these properties is crucial for analyzing quantum systems with similar characteristics.