Equation of motion for a rigid rotating rod

In summary, the problem is that you cannot treat the rod as a simple pendulum. You must use the rotational KE = 1/2Iω2, not 1/2Mv^2. Additionally, you have to use the Lagrangian formalism to derive the equation of motion.f
  • #1
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Hi all,

Homework Statement


My problem is a pretty basic one, in a exercise a rigid rod of mass M is rotating around a horizontal pivot point i one end. The rod has the length L. I now need to derive the equation of motion using the Lagrangian formalism.

My question is:
Can i view the rod as a pendulum with a bob mass equal to that of the rod?


In this case the equation would simply be:
[itex]\theta '' + \sqrt{\dfrac{g}{L}} sin(\theta)=0[/itex]

Best Regards
Cole.
 
  • #2
My question is:
Can i view the rod as a pendulum with a bob mass equal to that of the rod?
Not exactly. An extended mass such as a rod cannot be treated as a simple pendulum. Treat it as a physical (or compound) pendulum.
 
  • #3
Ach thanks your reference to compound pendulum got me on the right track.
It's all about the center of mass:
[itex]I \theta '' = -M_{cm} g L_{cm} sin \theta
\Leftrightarrow \theta '' = -\dfrac{3 g}{2 L} sin (\theta)[/itex]
 
  • #4
Good. Now do it using the Lagrangian. :smile:
 
  • #5
Thanks for the quick reply, I am slightly confused as how to in corporate the moment of inertia for the rod. If I use the kinetic energy [itex]T=\dfrac{1}{2}M r'^{2}[/itex] and potential energy [itex]U=-mg r \mathrm{cos} \theta[/itex] there is no difference from the regular pendulum and i don't get the 3/2 factor!
Could I use [itex]T=\dfrac{1}{2} I r'^{2}[/itex] where I is the inertia? A hint is appreciated :)

Regards
Cole.
 
  • #6
You must use the rotational KE = 1/2Iω2, not 1/2Mv^2. (You'll express in terms of θ', of course.)
 
  • #7
Great i figured it out!
However I have run into a new problem. Suppose the rod has a bead of mass m attached at the pivot moving down is it rotates. I can't figure out what the kinetic energy of the system is.. Me guess is [itex]T_{tot}=T_{rod}+T_{bead}=\dfrac{1}{2}\dot{\theta}^{2}\left( I_{rod}+I_{bead}\right) + \dfrac{1}{2}m\left( \dot{r}+r\dot{\theta}\right) ^2[/itex] because the bead must contribute with kinetic energy from the radial speed. ([itex]\bar{v}=v_{r}+v_{\theta}=\dot{r}+r\dot{\theta}[/itex]) However my equations of motion don't seem right.. Any hints? You've been more than helpful so far!

Regards
Cole.
 
  • #8
The KE of the rod is the same. Careful how you write the KE of the bead: Don't count it twice and don't add perpendicular velocity components together before squaring them.
 
  • #9
Everything appears correct except for the velocity factor. When I expand it I get:
[itex]\dfrac{1}{2}m\ddot{r}^{2}+m\dot{r}r\dot{\theta}+ \dfrac{1}{2} mr^{2}\dot{\theta}^{2}[/itex]
and when I use the part of the Legrender equation relevant for the energy I get:
[itex]\dfrac{\mathrm{d}}{\mathrm{t}}\dfrac{\mathrm{d}L}{\mathrm{d}\dot{\theta}}=m\dot{r}r\ddot{\theta} +m r^{2}\ddot{\theta}[/itex]
I have deduced from another solution that the above result should simply be: [itex] 2mr \dot{r} \dot{\theta} [/itex]
Where am I going wrong?
Thanks a million for the help!

Regards
Cole.
 
  • #10
Everything appears correct except for the velocity factor. When I expand it I get:
[itex]\dfrac{1}{2}m\ddot{r}^{2}+m\dot{r}r\dot{\theta}+ \dfrac{1}{2} mr^{2}\dot{\theta}^{2}[/itex]
What did you expand to get this? If you are referring to the last term in the following, I'd say it was wrong:
Me guess is [itex]T_{tot}=T_{rod}+T_{bead}=\dfrac{1}{2}\dot{\theta}^{2}\left( I_{rod}+I_{bead}\right) + \dfrac{1}{2}m\left( \dot{r}+r\dot{\theta}\right) ^2[/itex]
Reread my last post.
 
  • #11
Yes I am referring to the last term:
[itex]\dfrac{1}{2}m( \dot{r}+r \dot{\theta} )^{2}=\dfrac{1}{2}m(\dot{r}^{2}+2r\dot{r} \dot{\theta}+r^{2}\theta ^{2})[/itex]
What i think you mean in the above is to say:
[itex]T_{b}=\dfrac{1}{2}I_{b}\dot{\theta}+\dfrac{1}{2}m \dot{r} ^{2}+\dfrac{1}{2}mr^{2} \dot{\theta}^{2}[/itex]
but that doesn't either give me the expression I'm looking for..
 
  • #12
What i think you mean in the above is to say:
[itex]T_{b}=\dfrac{1}{2}I_{b}\dot{\theta}+\dfrac{1}{2}m \dot{r} ^{2}+\dfrac{1}{2}mr^{2} \dot{\theta}^{2}[/itex]
Yes, that's what I would put as the KE term. Except that Ib should be Irod in the first term. And the [itex]\dot{\theta}[/itex] should be squared.
but that doesn't either give me the expression I'm looking for..
Why is that?
 
  • #13
Ahh but it does! Silly mistake from my part.
Thank you so much it has been a real journey :)

Regards
Cole.
 

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