Angular velocity of rigid object

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Homework Help Overview

The discussion revolves around a problem involving the angular velocity of a rigid object, which is rotated about a specific axis. The total kinetic energy of the object is provided, along with the masses and dimensions of the components involved. Participants are trying to understand how to relate kinetic energy to angular velocity using the moment of inertia and other relevant equations.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the use of the kinetic energy equation KE=(1/2)IW² and the need to calculate the moment of inertia for the system. There are attempts to derive the moment of inertia for the individual masses and sum them up. Some participants question whether it is necessary to calculate the moment of inertia or if the problem can be approached directly using the kinetic energy formula in terms of angular velocity.

Discussion Status

The discussion is active, with participants providing different perspectives on the necessity of calculating the moment of inertia versus using the kinetic energy directly. Some guidance has been offered regarding the equations to use, but there is no explicit consensus on the best approach yet.

Contextual Notes

Participants are working under the assumption that the masses can be treated as point particles, and there is a focus on the relationship between linear and angular quantities. The problem setup includes specific values for mass and dimensions, which are critical to the calculations being discussed.

jhoffma4
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Hi I am having trouble with a problem that involves angular velocity. The problem states:

The rigid object shown is rotated about an axis perpendicular to the paper and through point P. The total kinetic energy of the object as it rotates is equal to 1.4 J. If M = 1.3 kg and L = 0.50 m, what is the angular velocity of the object? Neglect the mass of the connecting rods and treat the masses as particles.

There is an illustration that I tried to insert below...if it does not show, here is a description:

The object has a total of 4 spheres. The first 2 spheres are each of mass M and are attached to opposite ends of a rod whose length is 2L. The other 2 spheres are each of mass 2M and are attached to opposite ends of a rod whose length is L. The rods cross one another at their midpoints.

https://my.usf.edu/courses/1/PHY2048.801C08/ppg/examview/Chpater_img/mc025-1.jpg


The equations I was trying to use are:

KE=(1/2)IW^2 (I'm using W for angular velocity)
I also know KE=(1/2)mv^2 (for linear values) and v=WR.

I don't know where to go from here. Could someone help me?
 
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Use the first equation you provided KE=(1/2)IW^2. You know net KE = 1.4, so you have to figure out I (which = MR^2) for each sphere, sum up what you get and solve for W.
 
jhoffma4 said:
… treat the masses as particles.

The equations I was trying to use are:

KE=(1/2)IW^2 (I'm using W for angular velocity)
I also know KE=(1/2)mv^2 (for linear values) and v=WR.

Hi jhoffma4! :smile:

(have a squared: ² and an omega: ω)

You don't need I … the masses are particles, and you're not asked for the angular momentum anyway.

You only need the angular velocity to calculate the actual velocities. :smile:
 
cryptoguy,
I think I did what you suggested to do correctly...

To find I(net),
I1=I3=(M)(L²)
I2=I4=(2M)(L/2)²

--> I(net)= I1+I2+I3+I4
= 2[(M)(L²)] + 2[(2M)(L/2)²]

and then I plugged I(net) into the KE equation to solve for ω...I got 1.7.

Thank you!
 
thx for the symbols tinytim :)
 
hm looks right to me, I'm not sure off the top of my head how you can do this without I as tiny-tim said.
 
cryptoguy said:
hm looks right to me, I'm not sure off the top of my head how you can do this without I as tiny-tim said.

Hi cryptoguy! :smile:

Because the energy, which is given as 1.4J, is ∑(1/2)mv², = ∑(1/2)mω²r². :smile:

I don't understand how you get an I (unless you use the parallel axis theorem, with an I0 of 0).
 
well the moment of inertia of a point mass is mr² so in effect, ∑(1/2)mω²r² = ∑(1/2)Iω²
 
But why bother, when ∑(1/2)mω²r² is already what you want? :smile:
 
  • #10
tiny-tim said:
But why bother, when ∑(1/2)mω²r² is already what you want? :smile:

Given ∑(1/2)mω²r². Does that mean you solve the problem by setting it equal to Ke and solving for omega?
 

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