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McCoy13
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Homework Statement
The two weights on the left have equal masses m and ar connected by a massless spring of force constant k. The weight on the right has mass 2m, and the pulley is massless and frictionless. The coordinate x is the extension of the spring from its equilibrium length; that is, the length of the spring is l+x where l is the equilibrium length with all the weights in position and with the 2m weight held stationary.
Show that the total potential energy is just [itex]U=\frac{1}{2}kx^{2}[/itex]
Homework Equations
[tex]U_{grav}=mgh[/tex]
[tex]U_{spr}=\frac{1}{2}kx^{2}[/tex]
The Attempt at a Solution
Attempt 1 (ignoring all sorts of constants added onto potential energy, since they'll disappear in Lagrange's/Hamilton's equations):
[tex]U=2mgy-mgy-mg(y+l+x)+\frac{1}{2}kx^{2}[/tex]
[tex]U=-mgx+\frac{1}{2}kx^{2}[/tex]
(the l was dropped for the noted reason above)
Attempt 2 (preserving all constants incase I missed something):
let the length of the rope be L;
[tex]U=2mg(y-L)-mgy-mg(y+l+x)+\frac{1}{2}kx^{2}[/tex]
[tex]U=\frac{1}{2}kx^{2}-mgx-mg(2L+l)[/tex]
I turned up something on a Dutch forum about changing the quadratic in the bottom from the form Ax^2+Bx+C to something like Ax^2+D and then just letting D=0 (since constant adjustments of potential don't matter), but I have absolutely no idea how to do that and it seems kind of mathematically spurious that you can change a linear term into a constant.
Am I missing something here?