Lagrangian mechanics - rotating rod

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SUMMARY

The discussion focuses on the calculation of kinetic energy for a rotating rod within the framework of Lagrangian mechanics. It clarifies that both translational and rotational kinetic energy must be considered when calculating the total kinetic energy, particularly when the frame of reference is the center of mass. The conversation emphasizes the importance of understanding the configuration of the system, specifically a beam attached at one end, to accurately apply these principles. The mathematical representation of kinetic energy, expressed as ##\int {1\over 2} {\dot r}^2 \; dm\ ##, is highlighted as a key concept in this analysis.

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pj33
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Hello,

It might sound silly, but when I try to calculate the kinetic energy of a rotating rod to form the Langrangian (and in general), why it has both translational and rotational kinetic energy?

Is it because when I consider the moment of Inertia about the centre I need to include the translational since my "frame of reference" is the centre and it moves but when considering about end I only take into aacount the rotatioal since by "frame of reference" (end of rod) is stationary?

I am looking more for a physical interpretation/intuition.
I hope my explanation above is clear enough!

Thank you in advance!
 
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You talk about a stationary end of rod, so you must have some specific configuration in mind. Can you divulge to us what it is ?

Note that ##\int {1\over 2} {\dot r}^2 \; dm\ ## is the kinetic energy in all cases. Often it is convenient/ useful/ practical to split it up in parts, e.g. as in your c.o.m plus rotation. A force like gravity works on all ##dm## but can comfortably be considered to work on the c.o.m. that way.

All in all nothing physical, just a mathematical approach :wink:

##\ ##
 
BvU said:
You talk about a stationary end of rod, so you must have some specific configuration in mind. Can you divulge to us what it is ?

Note that ##\int {1\over 2} {\dot r}^2 \; dm\ ## is the kinetic energy in all cases. Often it is convenient/ useful/ practical to split it up in parts, e.g. as in your c.o.m plus rotation. A force like gravity works on all ##dm## but can comfortably be considered to work on the c.o.m. that way.

All in all nothing physical, just a mathematical approach :wink:

##\ ##
I was just thinking of a simple beam attached at one end at a stationary point.
If I understand this, it helps to tackle harder problems. Thank you!
 
pj33 said:
I was just thinking of a simple beam attached at one end at a stationary point.

That is a system with a constraint, so already not all that trivial, but surely instructive.

##\ ##
 

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