Uploaded March 2015 | Updated September 2026, 1 week ago
When we consider behavior of multi-electron systems we are faced with equations and mathematics that quickly become overwhelming. In 1929 Douglass Hartree described a way to approximate these interactions that made computation quantum chemistry practical.
The playlist: youtube.com/playlist?list=PL193BC0532FE7B02C
Part b: youtu.be/QludPcDLe1I
Comments, including questions, suggestions and constructive criticism are always welcome.
At 0:34 the subscript of the second Laplacian should be 2, not 1. It refers to the second electron.
When we consider behavior of multi-electron systems we are faced with equations and mathematics that quickly become overwhelming. In 1929 Douglass Hartree described a way to approximate these interactions that made computation quantum chemistry practical.
The playlist: youtube.com/playlist?list=PL193BC0532FE7B02C
Part b: youtu.be/QludPcDLe1I
Comments, including questions, suggestions and constructive criticism are always welcome.
At 0:34 the subscript of the second Laplacian should be 2, not 1. It refers to the second electron.

![Quantum Mechanics 7a - Angular Momentum I
Part b: http://youtu.be/7OmvPygd3iY
The solution of the Schrödinger for the hydrogen atom predicts electron orbitals indexed by three quantum numbers: n, l and m. Weve seen that n specifies the energy level. Here we find that l and m tell us what it is possible to know about the atoms angular momentum.
[ratings and comments are always welcome]
The playlist: http://www.youtube.com/playlist?list=PL193BC0532FE7B02C
The following image was used under the Creative Commons license
http://commons.wikimedia.org/wiki/File:Schrodingers_cat.svg by Dhatfield CC-by-SA 3.0 Quantum Mechanics 7a - Angular Momentum I](https://i.ytimg.com/vi/NwbvTa2xV9k/mqdefault.jpg)








