Go to the U of M home page
School of Physics & Astronomy
School of Physics and Astronomy Wiki

User Tools


classes:2009:fall:phys4101.001:quiz_3_1113

Differences

This shows you the differences between two versions of the page.

Link to this comparison view

Both sides previous revisionPrevious revision
classes:2009:fall:phys4101.001:quiz_3_1113 [2009/11/12 23:19] x500_chap0326classes:2009:fall:phys4101.001:quiz_3_1113 [2009/11/13 09:23] (current) x500_maxwe120
Line 45: Line 45:
 ===physics4dummies 11/12 8:30pm=== ===physics4dummies 11/12 8:30pm===
 Been doing the practice test and I need to know if problem 2 is as easy as plugging the change of coordinates into the operator equation.  Been doing the practice test and I need to know if problem 2 is as easy as plugging the change of coordinates into the operator equation. 
 +
 +==Zeno 9am 11/13==
 +Generally, yes, but since the x and y momentum operators involves derivatives of x and y respectively you need to change the derivatives from Cartesian to spherical coordinates. You can do this by exploiting the chain rule for derivatives and obtaining 
 +
 + <math>\frac{\partial}{\partial x}= \frac{\partial \rho}{\partial x} \frac{\partial}{\partial \rho} + 
 + \frac{\partial \theta}{\partial x} \frac{\partial}{\partial \theta} +
 + \frac{\partial \phi}{\partial x} \frac{\partial}{\partial \phi} </math>
 +
 +Then just use the definitions for the change of coordinates to compute each respective component derivative and you'll be left with spherical coordinate derivative operators multiplied by variables on to the left. If you do it correctly you'll obtain equation 4-129.
  
 ===Ekrpat 1135=== ===Ekrpat 1135===
classes/2009/fall/phys4101.001/quiz_3_1113.1258089564.txt.gz · Last modified: 2009/11/12 23:19 by x500_chap0326