Rolling Motion of a Rigid Object

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SUMMARY

The discussion focuses on the rolling motion of a uniform solid disk and a uniform hoop released from rest on an incline of height h. Using conservation of energy, the participants derive the speeds of both objects when they reach the bottom, emphasizing the importance of rotational inertia (I) in the calculations. The moment of inertia for the hoop is given as I = MR², while for the disk it is I = (1/2)MR². The conclusion drawn is that the disk will reach the bottom first due to its lower moment of inertia compared to the hoop.

PREREQUISITES
  • Understanding of conservation of energy principles in physics
  • Familiarity with rotational inertia and its formulas
  • Knowledge of kinematics related to rolling motion
  • Basic trigonometry to relate height and incline angle
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  • Calculate the speeds of different objects using their respective moments of inertia
  • Explore the effects of friction on rolling motion
  • Study the dynamics of rolling objects on varying incline angles
  • Learn about the energy conservation in non-conservative systems
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Students of physics, educators teaching mechanics, and anyone interested in understanding the dynamics of rigid body motion and energy conservation principles.

APool555
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I have no clue where to start on this problem. I appreciate any help. Thanks.

A uniform solid disk and a uniform hoop are placed side by side at the top of an incline of height h. If they are released from rest and roll without slipping, which object reaches the bottom first? Verify you answer by calculating their speeds when they reach the bottom in terms of h.
 
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We assume no friction ? No ? Ok then use conservation of energy :

MgLsin( \theta) = \frac{1}{2}I \omega^2 + \frac{1}{2}Mv^2

v is the speed, omega the angular speed and L is the length of the incline which makes an angle theta with the horizontal.

The clue really is to see the motion of a rigid object as the sum of a translation and a rotation : hence the two terms on the RHS, which express the kinetic energy

Keep in mind that v = \omega R where R is the radius of the object

Just fill in the I (rotational inertia about the center of mass of the rotating object) for both objects and solve for v so you can compare

oh i just realized, the Lsin(theta) is equal to the height h...so you can replace them...

marlon
 
Last edited:
Ok, I can see that now. h=Lsin(theta)

How do I fill in the I for both objects when I'm given no values at all?
 
APool555 said:
Ok, I can see that now. h=Lsin(theta)

How do I fill in the I for both objects when I'm given no values at all?

They should have been given. You can calculate them yourselves by using 3-D-integration, but let's keep it simple

For the hoop I = MR²
For the disk I = (1/2)MR²
For a sphere I =(2/5)MR²

So assume all objects have same radius R and same mass M, which one will come down first and which one last ?

Be sure you write v as a function of h, I and R and then substitute the I-values for each object...


marlon
 
Last edited:
Marlon said:
(...) For a sphere I =(2/5)MR²(...)



*For a 2-sphere of mass M & radius R,the moment of inertia wrt a rotation axis (chosen as Oz) passing through the center of the 2-sphere is

I_{Oz}^{2-sphere} = \frac{2MR^{2}}{3}

*For a ball in \mathbb{R}^{3} of mass M and radius R,the moment of inertia wrt a rotation axis (chosen as Oz) passing through the center of the ball is

I_{Oz}^{ball \subset \mathbb{R}^{3}} =\frac{2MR^{2}}{5}


Daniel.
 
dextercioby said:
*For a 2-sphere of mass M & radius R,the moment of inertia wrt a rotation axis (chosen as Oz) passing through the center of the 2-sphere is

:smile: :smile: :smile: :smile:

What the hell is a two dimensonal sphere ?
You are talking about a spherical shell...that is not the same...aahhhhh

TO the OP : let's also study the spherical shell... :smile:

marlon
 
A 2-sphere...yes yes yes :) :) :)

marlon
 
2-Sphere is the surface of (implicit) equation (in cartesian coordinates)

x^{2}+y^{2}+z^{2}=R^{2}

and it's not funny not to know what a 2-sphere is...:rolleyes:

Daniel.
 

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