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classes:2009:fall:phys4101.001:q_a_1104 [2009/11/10 00:26] mbryanclasses:2009:fall:phys4101.001:q_a_1104 [2009/12/19 16:56] (current) x500_sohnx020
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-===== Nov 04 (Wed)  =====+===== Nov 04 (Wed) Laplacian in spherical coordinate, Legendre =====
 **Return to Q&A main page: [[Q_A]]**\\ **Return to Q&A main page: [[Q_A]]**\\
 **Q&A for the previous lecture: [[Q_A_1102]]**\\ **Q&A for the previous lecture: [[Q_A_1102]]**\\
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 **Main class wiki page: ** [[home]] **Main class wiki page: ** [[home]]
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 ====Ekrpat 1144 12:50pm==== ====Ekrpat 1144 12:50pm====
 A simple question about tuesday's discussion.  When solving for the eigenvector for the second and third eigenstate, I am getting A simple question about tuesday's discussion.  When solving for the eigenvector for the second and third eigenstate, I am getting
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 ====Dark Helmet 11/05==== ====Dark Helmet 11/05====
 Although i understand how to get them, what exactly is the physical interpretation of eigenstates and eigenvalues?  That still is confusing me a bit. Although i understand how to get them, what exactly is the physical interpretation of eigenstates and eigenvalues?  That still is confusing me a bit.
 +
 +=== Blackbox ===
 +In quantum mechanics, operators correspond to observable variables, eigenvectors are also called eigenstates, and the eigenvalues of an operator represent those values of the corresponding variable that have non-zero probability of occurring. In other words, we can say some special wave functions are called eigenstates, and the multiples are called eigenvalues. I hope this helped.
  
  
classes/2009/fall/phys4101.001/q_a_1104.1257834386.txt.gz · Last modified: 2009/11/10 00:26 by mbryan