Campuses:
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classes:2009:fall:phys4101.001:q_a_1123 [2009/11/23 17:36] – x500_porte210 | classes:2009:fall:phys4101.001:q_a_1123 [2009/11/28 22:18] (current) – ely | ||
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- | ===== Nov 23 (Mon) ===== | + | ===== Nov 23 (Mon) Spin operators, probabilities, |
**Return to Q&A main page: [[Q_A]]**\\ | **Return to Q&A main page: [[Q_A]]**\\ | ||
**Q&A for the previous lecture: [[Q_A_1120]]**\\ | **Q&A for the previous lecture: [[Q_A_1120]]**\\ | ||
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**Main class wiki page: ** [[home]] | **Main class wiki page: ** [[home]] | ||
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====Daniel Faraday 11/22 6pm==== | ====Daniel Faraday 11/22 6pm==== | ||
In the proof that [L^2,Lx] = 0 on page 161, how does Griffiths get from the first line to the second line? | In the proof that [L^2,Lx] = 0 on page 161, how does Griffiths get from the first line to the second line? | ||
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Cathode ray tubes (http:// | Cathode ray tubes (http:// | ||
+ | == Zeno 11/25 9am == | ||
+ | I knew there was something obvious that I was overlooking. Thanks! | ||
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+ | ===David Hilbert' | ||
+ | As far as I know they actually cooked silver atoms from a furnace. Wikipedia mentions that you need to have particles with a total electric charge of zero because otherwise they would deflect under the influence of a magnetic field before coming out of the apparatus - http:// | ||
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+ | ===David Hilbert' | ||
+ | Also http:// | ||
- | ====John Galt | + | ===Dark Helmet |
- | Does anyone see anything useful coming from taking the time derivative of A(t) and B(t) as described in class and setting | + | I don't know if it is exactly the same thing, but a free-electron laser would be a beam of electrons. |
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