At this level of discussion, I seriously doubt that going further is fruitful. This gets across an important point.
Unfortunately, it also gives an illusion of understanding, since it does not explain that this is only one example out of many (why do different components of momentum commute, but different components of angular momentum do not?). As for the Fourier transform, arguably this can be presented as a result of position and momentum being conjugate variables/canonical coordinates. Speaking of which, any pair of classical canonical variables probably translates into a version of uncertainty relation, even such unusual ones as action/angle, fluxes of electric and magnetic fields, etc.
Good catch on angle/angular momentum. Obvious now that you point it out.
"Illusion of understanding" - I don't see what's so illusory about understanding one case - the most commonly met case, the one people hear about and get confused by.
If one has looked into quantum mechanics enough to know about the other cases, and understands the position/momentum connection, but can't figure out the nature of the relationship of these other cases... such a person is sufficiently black-swan-ish that I don't believe failure to account for em when writing the sequence was really a deficiency.
Today's post, The So-Called Heisenberg Uncertainty Principle was originally published on 23 April 2008. A summary (taken from the LW wiki):
Discuss the post here (rather than in the comments to the original post).
This post is part of the Rerunning the Sequences series, where we'll be going through Eliezer Yudkowsky's old posts in order so that people who are interested can (re-)read and discuss them. The previous post was Decoherence, and you can use the sequence_reruns tag or rss feed to follow the rest of the series.
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