Conceptual questions about rotational dynamics.

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Homework Help Overview

The discussion revolves around a problem involving a dumbbell with two unequal masses rotating about a point. The original poster seeks to understand how to change the distance between the masses to double the rotational kinetic energy while keeping the angular velocity constant. There are also conceptual questions regarding the moment of inertia of non-rotating objects.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive a relationship between the distance R and the rotational kinetic energy, leading to confusion about the factor by which R must change. Some participants suggest setting up equations for kinetic energy and solving for R. Others question the assumptions about moment of inertia for non-rotating objects.

Discussion Status

Participants are actively engaging with the problem, providing different approaches to clarify the misunderstanding regarding the factor by which R must change. There is a recognition of the importance of understanding the relationship between kinetic energy and distance, with some guidance offered on systematic problem-solving methods.

Contextual Notes

There is an ongoing discussion about the definitions and implications of moment of inertia, particularly in relation to objects that are not in motion. The original poster expresses uncertainty about their understanding and seeks confirmation on the preferred methods for solving such problems.

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Homework Statement


There is a dumbbell with two masses attached at each end, rotating about a point. The distance between the two masses is R, and the two masses do not have the same mass. m1 < m2

If the angular velocity ω is held constant, by what factor must R change to double the rotational kinetic energy of the dumbbell?

Homework Equations


[itex]I = mr^{2}[/itex]
[itex]r = \frac{R}{2}[/itex]
[itex]K_{rot} = \frac{1}{2}I\omega^{2}[/itex]

The Attempt at a Solution


Since [itex]r = \frac{R}{2}[/itex] and [itex]I = (m_{1}+m_{2})r^{2}[/itex], then [itex]K_{rot} = \frac{1}{2}[(m_{1}+m_{2})((\frac{R}{2})^{2})]\omega^{2} =>\frac{1}{2}[(m_{1}+m_{2})(\frac{R^{2}}{4})]\omega^{2}[/itex]

If Rotational kinetic energy is doubled and angular velocity is to be constant, then:
[itex]2K_{rot} = 2(\frac{1}{2}[(m_{1}+m_{2})(\frac{R^{2}}{4})]\omega^{2})[/itex]
[itex]2K_{rot} = \frac{1}{2}[(m_{1}+m_{2})(\frac{2R^{2}}{4})]\omega^{2}[/itex]
[itex]2K_{rot} = \frac{1}{2}[(m_{1}+m_{2})(\frac{R^{2}}{2})]\omega^{2})[/itex]

Thus, by my conclusion, R increases by a factor of two if the rotational energy is doubled but angular velocity is to remain constant. My book's answer is that R increases by a factor of square root of 2. What did I do wrong?

Also, one more conceptual question: If an object is not rotating, does it have a moment of inertia? The answer is no, correct? Since a moment of inertia depends on the rotation of axis and changes when an object is rotating about a different point, thus if an object is not rotating, then it does not have a moment of inertia since moment of inertia is the rotational equivalent of mass.
 
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Retribution said:
Thus, by my conclusion, R increases by a factor of two if the rotational energy is doubled but angular velocity is to remain constant. My book's answer is that R increases by a factor of square root of 2. What did I do wrong?
Try this:
KE1 = f(R1)
KE2 = f(R2)
Set KE2 = 2KE1 and then solve for R2 in terms of R1.

Also, one more conceptual question: If an object is not rotating, does it have a moment of inertia? The answer is no, correct? Since a moment of inertia depends on the rotation of axis and changes when an object is rotating about a different point, thus if an object is not rotating, then it does not have a moment of inertia since moment of inertia is the rotational equivalent of mass.
If an object isn't moving does it still have mass? Same idea here. Of course it has a moment of inertia (which depends on the axis you choose to rotate about).
 
Doc Al said:
Try this:
KE1 = f(R1)
KE2 = f(R2)
Set KE2 = 2KE1 and then solve for R2 in terms of R1.
The major mistake I made was to assume that R denoted the length, not the radius. In that case:
[itex]\frac{1}{2}(m_{1} + m_{2})(R_{2})^{2}\omega^{2} =2[\frac{1}{2}(m_{1} + m_{2})(R_{1})^{2}\omega^{2}][/itex]
Masses and angular velocity cancels out:
[itex]\frac{1}{2}(R_{2})^{2} =2[\frac{1}{2}(R_{1})^{2}][/itex]
[itex]R_{2} = \sqrt{2R_{1}}[/itex]

Thanks for all the help. I just wanted to know, is this the preferred method of going about solving these types of questions? I would usually plug in numbers, but that method mislead me into thinking I had the right answer.
Doc Al said:
If an object isn't moving does it still have mass? Same idea here. Of course it has a moment of inertia (which depends on the axis you choose to rotate about).
Ah, I see. Thanks.
 
Retribution said:
Thanks for all the help. I just wanted to know, is this the preferred method of going about solving these types of questions? I would usually plug in numbers, but that method mislead me into thinking I had the right answer.
It's how I would approach a problem like this. The main thing is to realize that the KE is proportional to R2. So to double the KE you need to multiply R by √2.

But doing it systematically reduces the chance for error. (And may lead to a deeper understanding.)
 

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