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Assignment #3 for the classical mechanics i course (ph 461/561) taught at the university of alabama at birmingham in the fall of 2005. The assignment includes problems related to calculating work done by a force in different situations and discussing the physical meaning of the results. It also includes problems related to the force f(x) = 4c(x^3 - x) and its effect on the total mechanical energy of a particle.
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PH 461/561 – Classical Mechanics I – Fall 2005
Assignment # 3 Due: Thursday, September 1 (Turn in for credit!)
Activities based on previous lecture:
a positive constant (i.e., a force linear on the position x ).
Calculate the work done by this force in the three different situations below.
a. When particle moves in configuration space from point a to point b according to the following orbit:
b. When particle moves in configuration space from point a to point b according to the following orbit:
c. When particle moves in configuration space from point a to point b according to the following orbit:
d. Compare the values you found for the work in situations (a), (b), (c) and discuss the meaning of your finding.
a b (^) x
a b c x
a u s b (^) x
is a positive constant and v is the particle velocity. Assume that at point x=a the particle has an initial velocity v 0 , and that b ≤ a + mv α^0.
Calculate the work done by this force in the three different situations below.
a. Calculate the work done by this force when the particle moves in configuration space from point a to point b according to the following orbit:
b. Discuss the physical meaning of the result you found for the work in part (a). Your discussion should focus on the following aspects:
i. Showing that the work done by F(v) does NOT depend only on the end points a and b.
ii. Showing that the work done by F(v) depends on how the particle moves from a to b (i.e., the work depends on the history , on the details of the orbit in configuration space, on the details of the path in one dimension, etc.).
c. Explain what happens with the work done by F(v) in the following limiting cases:
i. When b = a. What is the physical meaning of this situation?
ii. When b = a + mv α^0. What is the physical meaning of this situation?
a b (^) x