{"id":498,"date":"2016-11-03T19:53:44","date_gmt":"2016-11-04T02:53:44","guid":{"rendered":"https:\/\/sites.evergreen.edu\/psam1617\/?p=498"},"modified":"2016-11-03T19:57:57","modified_gmt":"2016-11-04T02:57:57","slug":"classical-mechanics-homework-assignment-11","status":"publish","type":"post","link":"https:\/\/sites.evergreen.edu\/psam1617\/classical-mechanics-homework-assignment-11\/","title":{"rendered":"Classical Mechanics Homework Assignment #11"},"content":{"rendered":"

Classical Mechanics Homework Assignment #11, due <\/del>by 5 pm Monday November 7 to Krishna’s office Lab 2 3255<\/span>. All problems from Taylor except as indicated.
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  1. Choose one of 7.20, 7.22, or 7.23 that you didn’t do for Homework #10<\/a><\/strong><\/li>\n
  2. Choose one of 7.29, 7.30, or 7.35 that you didn’t do for Homework #10<\/a><\/strong><\/li>\n
  3. 7.50<\/li>\n
  4. 7.52 (see note)<\/li>\n
  5. Consider a simple pendulum with mass m<\/em> and (massless) string of length b<\/em>, released from rest at an angle \u03b8<\/em>0<\/sub> with respect to vertical. Determine the tension in the string as a function of angle \u03b8<\/em> and other given and known constants. Check that your answer makes sense in the limit cases when \u03b8 <\/em>= \u03b8<\/em>0<\/sub> (i.e. at the top of the swing) and when \u03b8<\/em> = 0 (the bottom of the swing). This is the problem we discussed in class; recall from that discussion that we could only get so for with the Lagrangian method, so don’t hesitate to use a Newtonian framework as needed. (see note)<\/li>\n
  6. There are only five problems on this homework set.<\/li>\n<\/ol>\n

    Notes:<\/p>\n