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Bohemian Gravity

Posted: Tue Sep 17, 2013 4:20 pm
by neufer
Click to play embedded YouTube video.

Re: Bohemian Gravity

Posted: Tue Sep 17, 2013 4:58 pm
by geckzilla
I hereby crown this man Nerd of the Year 2013... there's not a chance anyone else can even compete at this point. There's no way I could even get past watching videos of my own face for entire days at a time.

Re: Bohemian Gravity

Posted: Tue Sep 17, 2013 5:13 pm
by BMAONE23
Neuf,
That was so good, I had to pass it on

Re: Bohemian Gravity

Posted: Tue Sep 17, 2013 8:26 pm
by Beyond
In keeping with the Gravity of the situation, i don't know what to say. He seems to be way 'beyond' me. :lol2:

Re: Bohemian Gravity

Posted: Tue Sep 17, 2013 9:12 pm
by orin stepanek
Czech it out; Bohemian Gravity yet! 8-) too deep for me though! :D

Re: Bohemian Gravity

Posted: Tue Sep 17, 2013 9:47 pm
by neufer
geckzilla wrote:
I hereby crown this man Nerd of the Year 2013...
Is that more prestigious than being Goofball of the Year :?:

Re: Bohemian Gravity

Posted: Tue Sep 17, 2013 10:16 pm
by geckzilla
Possibly.

Re: Bohemian Gravity

Posted: Tue Jun 16, 2020 5:12 pm
by neufer
geckzilla wrote: ↑Tue Sep 17, 2013 4:58 pm


I hereby crown this man Nerd of the Year 2013...
there's not a chance anyone else can even compete at this point.

There's no way I could even get past watching videos of my own face for entire days at a time.
https://en.wikipedia.org/wiki/Path_integral_formulation wrote:

<<The basic idea of the path integral formulation can be traced back to Norbert Wiener, who introduced the Wiener integral for solving problems in diffusion and Brownian motion. This idea was extended to the use of the Lagrangian in quantum mechanics by Paul Dirac in his 1933 article. The complete method was developed in 1948 by Richard Feynman. Some preliminaries were worked out earlier in his doctoral work under the supervision of John Archibald Wheeler. The original motivation stemmed from the desire to obtain a quantum-mechanical formulation for the Wheeler–Feynman absorber theory using a Lagrangian (rather than a Hamiltonian) as a starting point.