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Mechanics}Hamiltonian

The Hamiltonian is just the sum of the kinetic and potential energy, H=T+V.

The kinetic energy due to each mass is T_i = p_i^2/(2m). The potential energy is just U=1/2 k (\Delta l)^2. \Delta l = l -l_0, and thus factoring out the 1/2, one arrives at choice (E).

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Comments
jmason86
2009-07-05 20:04:03
If you didn't know the potential energy of the spring, you could derive it from Hooke's law.

F = -kx
In general, U=\int F, so
U = -\frac{1}{2}kx^2

What I don't get is that the negative in Hooke's law doesn't just disappear because you integrate.. so why is potential energy stored in a spring defined to be positive? This would lead to the incorrect answer of (D).
jmg810
2009-07-08 14:19:25
If a force is derivable from a position dependent potential\,U then \vec{F} = -\nabla{U}(\vec{r}), and hence \,U = -\int{F}\,d\vec{r}.
jmg810
2009-07-09 09:20:29
Typo fix:

\,U = -\int\vec{F}\cdot\,d\vec{r}
jmason86
2009-07-23 17:36:11
Thanks!
NEC
neutrino
2007-10-31 03:34:57
I don't understand the signs. If the string is ``fully stretched", T=0, but V is max. I would guess answer D in this case.

What is my error?
hot_dark_matter
2008-05-23 15:00:49
If the spring is fully stretched, it doesn't mean that the kinetic energy is zero. Presumably, the directions of \mathbf{p}_1 and \mathbf{p}_2 indicate the system can have translational and rotational energy.

As for the signs, kinetic energy is always positive and so is the potential energy stored by a spring. This eliminates all choices but (B) and (E). Given that there is only one spring, the answer must be (E).
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