Difference between revisions of "Schrödinger's equation"
Jump to navigation
Jump to search
(Created page with ": $$i \hbar \frac{\partial \psi}{\partial t} = - \frac{\hbar^2}{2 m} \nabla^2 \psi + V \psi$$ == Resources: == *[https://en.wikipedia.org/wiki/Schr%C3%B6dinger_equation Schr...") |
|||
(3 intermediate revisions by 2 users not shown) | |||
Line 1: | Line 1: | ||
'''Erwin Schrödinger''' (b. 1887) | |||
'''''Schrödinger equation''''' 1925 | |||
The Schrödinger equation is a linear partial differential equation that describes the wave function or state function of a quantum-mechanical system. | |||
: $$i \hbar \frac{\partial \psi}{\partial t} = - \frac{\hbar^2}{2 m} \nabla^2 \psi + V \psi$$ | : $$i \hbar \frac{\partial \psi}{\partial t} = - \frac{\hbar^2}{2 m} \nabla^2 \psi + V \psi$$ | ||
Line 6: | Line 12: | ||
== Discussion: == | == Discussion: == | ||
[[Category:Pages for Merging]] |
Latest revision as of 17:39, 1 November 2020
Erwin Schrödinger (b. 1887)
Schrödinger equation 1925
The Schrödinger equation is a linear partial differential equation that describes the wave function or state function of a quantum-mechanical system.
- $$i \hbar \frac{\partial \psi}{\partial t} = - \frac{\hbar^2}{2 m} \nabla^2 \psi + V \psi$$