The proportion of kinetic energy of a rotating rigid body?

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Discussion Overview

The discussion centers on the kinetic energy of a rotating rigid body, specifically how to determine the proportion of translational kinetic energy to rotational kinetic energy. Participants explore various scenarios and factors that influence this proportion, including mass distribution and motion characteristics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants state that the kinetic energy of a rotating rigid body is expressed as K=1/2mv^2 + 1/2Iw^2 and inquire about calculating the proportion of translational and rotational energy.
  • It is proposed that the proportion depends on the object's characteristics and how energy is imparted to it, with some arguing that a more concentrated mass distribution leads to more translational energy.
  • One participant challenges the generality of the claim regarding mass distribution, citing a hoop as an example where the mass is not concentrated at the center.
  • Another participant emphasizes that the proportion is arbitrary without specifying the motion of the body, suggesting various scenarios such as rolling without slipping on different surfaces.
  • Discussion includes examples like a wheel rolling down an inclined plane, noting that gravitational potential energy (GPE) converts to kinetic energy (KE) and that the moment of inertia plays a crucial role in determining the relationship between translational and rotational speeds.
  • It is mentioned that the moment of inertia can be expressed as I=f·MR^2, where f depends on mass distribution.
  • One participant asserts that the proportion is determined by nature rather than through calculation, highlighting that the rate of translational movement is limited by rotational movement in certain scenarios.

Areas of Agreement / Disagreement

Participants express differing views on how to determine the proportion of translational to rotational kinetic energy, with no consensus reached on a specific theorem or method for calculation. Multiple competing perspectives on the influence of mass distribution and motion characteristics remain evident.

Contextual Notes

Participants note that the relationship between translational and rotational speeds is contingent on the specific motion of the body, which has not been uniformly defined across the discussion.

Jason Ko
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The kinetic energy of a rotating rigid body is given by K=1/2mv^2 + 1/2Iw^2 but how to determine the proportion of translational energy and rotational energy? I know that if the mass distribution is more concentrated at its center mass, then more energy goes to the translational part. But is there actually a theorem account for it and how do we actually calculate the proportion?
 
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Jason Ko said:
The kinetic energy of a rotating rigid body is given by K=1/2mv^2 + 1/2Iw^2 but how to determine the proportion of translational energy and rotational energy?
The proportion of translational and rotational kinetic energy depends on the object and how the energy is imparted to it.
Jason Ko said:
I know that if the mass distribution is more concentrated at its center mass, then more energy goes to the translational part.
No not in general. Take the extreme example of a hoop that has no mass at its center.
 
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Jason Ko said:
But is there actually a theorem account for it and how do we actually calculate the proportion?
The proportion depends on the motion of the body, which you have not specified, so it's completely arbitrary.
 
Jason Ko said:
The kinetic energy of a rotating rigid body is given by K=1/2mv^2 + 1/2Iw^2 but how to determine the proportion of translational energy and rotational energy? I know that if the mass distribution is more concentrated at its center mass, then more energy goes to the translational part. But is there actually a theorem account for it and how do we actually calculate the proportion?
As @A.T. says, you have to know how the body is moving -- how is ##\omega## related to ##v##?

Is it rolling without slipping on its [round] perimeter? So that ##v = \omega r##?

Is it rolling without slipping on some extended framework? So that ##v = \omega R## with ##R > r##?

Is it rolling without slipping on a slender axle while the bulk of the body extends further out? So that ##v = \omega R## with ##R < r##?

Is it a flywheel mounted on a vehicle with a gear drive so that ##v = k \omega## for some ##k## that depends on the gear ratio?

Is it even round?

Is it flying through space on a ballistic trajectory so that ##v## and ##\omega## have no relationsip at all?
 
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gleem said:
The proportion of translational and rotational kinetic energy depends on the object and how the energy is imparted to it.

No not in general. Take the extreme example of a hoop that has no mass at its center.
A wheel rolling down an inclined plane without slipping. The GPE converts to KE.
 
Jason Ko said:
A wheel rolling down an inclined plane without slipping. The GPE converts to KE.
You will still need the moment of inertia which depends on how the mass of the wheel is distributed. But once you have that, if the wheel is rolling without slipping then the translational and rotational speeds are related as @jbriggs444 said above: ##v=\omega r## and a bit of algebra will find the relationship between them.
 
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It's useful to write the moment of inertia as ##I=f\cdot MR^2##,
where ##f## is determined by the distribution of mass.
 
Jason Ko said:
The kinetic energy of a rotating rigid body is given by K=1/2mv^2 + 1/2Iw^2 but how to determine the proportion of translational energy and rotational energy?
We don't determine that proportion, nature does.

Jason Ko said:
A wheel rolling down an inclined plane without slipping. The GPE converts to KE.
In the case of a wheel rolling down an inclined plane without slipping, the rate of the translational movement is restricted or limited by the rate of the rotational one.
It will take more energy to initiate the rotation of any wheel that has a huge moment of inertia; therefore, the translational movement will be necessarily slow.

Please, see:
http://hyperphysics.phy-astr.gsu.edu/hbase/sphinc.html#sph

http://hyperphysics.phy-astr.gsu.edu/hbase/hoocyl.html#hc2

 

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