ing_it
- 27
- 1
Homework Statement
We have a rod (length L, mass m) suspended at a point whose distance from the center of mass is a.
1) prove that (generally) there exist two values of a (a1, a2) for which the pendulum oscillates with the same period.
2) derive and explain: T = 2\pi\sqrt{\frac{a_1+ a_2}{g}}
3) with what value of a do we get the smallest period?
2) derive and explain: T = 2\pi\sqrt{\frac{a_1+ a_2}{g}}
3) with what value of a do we get the smallest period?
Homework Equations
E = 1/2 I w^2
J= J^* + ma^2
J= 1/12 mL^2 + ma^2
T = 2\pi\sqrt{\frac{J}{mga}}
T = 2\pi\sqrt{\frac{L}{g}}
The Attempt at a Solution
1) I thought that two periods being the same would mean T1 = T2
2\pi\sqrt{\frac{J_1}{mga}}= 2\pi\sqrt{\frac{J_2}{mga}}
J^* + ma_1^2 =J^* + ma_2^2
a_1^2 =a_2^2
a_1 = +/- a_2
and since a1 = a2 would be the same location a1 = - a2 which would mean that the only way to get the same period for two different values of a, would be to have the a be the same but in different directions from the center of mass.
2) I noticed that T = 2\pi\sqrt{\frac{a_1+ a_2}{g}} looks a lot like T = 2\pi\sqrt{\frac{L}{g}}
So I thought that a1 + a2 = L
and that that would mean that the rod would be suspended on one end and the mass would be concentrated on the other end of the rod? I guess it sounds silly but I just couldn't figure out anything else.
3) \lim_{x\rightarrow 0} T = 2\pi\sqrt{\frac{J}{mga}} = 2\pi\sqrt{\frac{1/12 L^2 + a^2}{ga}}
since 2\pi\sqrt{\frac{1}{g}} is a constant I'll derive the rest because a limit is just a special type of derivation (I think?)
\frac{1/2 L^2 + a^2}{a} derived is:
La + a^2 + {\frac {L^2}{2}}
and from that I can see that the smaller the a the smaller the period of the oscillation so we would get the shortest period if the pendulum was hung from its center of mass.I was told my solution is wrong. I don't know which parts, I don't know why and I don't know how to correct it. If you could help me out somehow I'd be really grateful.
2\pi\sqrt{\frac{J_1}{mga}}= 2\pi\sqrt{\frac{J_2}{mga}}
J^* + ma_1^2 =J^* + ma_2^2
a_1^2 =a_2^2
a_1 = +/- a_2
and since a1 = a2 would be the same location a1 = - a2 which would mean that the only way to get the same period for two different values of a, would be to have the a be the same but in different directions from the center of mass.
2) I noticed that T = 2\pi\sqrt{\frac{a_1+ a_2}{g}} looks a lot like T = 2\pi\sqrt{\frac{L}{g}}
So I thought that a1 + a2 = L
and that that would mean that the rod would be suspended on one end and the mass would be concentrated on the other end of the rod? I guess it sounds silly but I just couldn't figure out anything else.
3) \lim_{x\rightarrow 0} T = 2\pi\sqrt{\frac{J}{mga}} = 2\pi\sqrt{\frac{1/12 L^2 + a^2}{ga}}
since 2\pi\sqrt{\frac{1}{g}} is a constant I'll derive the rest because a limit is just a special type of derivation (I think?)
\frac{1/2 L^2 + a^2}{a} derived is:
La + a^2 + {\frac {L^2}{2}}
and from that I can see that the smaller the a the smaller the period of the oscillation so we would get the shortest period if the pendulum was hung from its center of mass.I was told my solution is wrong. I don't know which parts, I don't know why and I don't know how to correct it. If you could help me out somehow I'd be really grateful.
Last edited: