Calculating the Speed of Hoops: A Physics Problem

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Homework Help Overview

The discussion revolves around a physics problem involving two rigidly fastened hoops, one smaller and one larger, released from a certain position. The objective is to determine the speed of the center of the larger hoop relative to the table when the centers of both hoops align vertically. The problem involves concepts from rotational dynamics, energy conservation, and moment of inertia.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of the center of mass and the moment of inertia for the system. There are attempts to apply energy conservation principles, and some participants question the correctness of the moment of inertia used in the calculations. Others suggest exploring the relationship between the velocities of the two hoops and the center of mass approach.

Discussion Status

The discussion is ongoing, with participants exploring different approaches to the problem. Some guidance has been offered regarding the use of the parallel axis theorem to find the moment of inertia about the center of mass. There is no explicit consensus yet, as participants are still evaluating their methods and assumptions.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information available and the methods they can employ. There is an emphasis on understanding the relationship between the components of the system and their respective motions.

John O' Meara
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Suppose in the figure attached View attachment Doc1.doc that the two hoops are rigidly fastened together. The system is released from the position shown and there is negligible friction between the large hoop and the table. How fast relative to the table is the center of the large hoop moving when the centers of the two hoops lie on a vertical line? If the radius of the small hoop is b and its mass is m and the radius of the large hoop =3b and its mass is 3m.
My attempt: If x=0 is the present position of the hoops then their center of mass is x_cm = -b/2. I=I1+I2=3*m*(3b)^2 + m*b^2 = 28*m*b^2.
Ug = Ktrans +Krot
4*m*g*b/2 = .5*4*m*v^2 + .5*I*v^2/(-b/2)^2
2*m*g*b = 2*m*v^2 + 2*28*b^2*v^2/b^2
= 2*m*v^2 + 56*m*v^2. Therefore 29*v^2=g*b. Therefore v = (g*b/29)^.5;
Is this the correct answer, if not where did I go wrong? Thanks.
 
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John O' Meara said:
Suppose in the figure attached View attachment 8109 that the two hoops are rigidly fastened together. The system is released from the position shown and there is negligible friction between the large hoop and the table. How fast relative to the table is the center of the large hoop moving when the centers of the two hoops lie on a vertical line? If the radius of the small hoop is b and its mass is m and the radius of the large hoop =3b and its mass is 3m.
My attempt: If x=0 is the present position of the hoops then their center of mass is

x_cm = -b/2

I=I1+I2=3*m*(3b)^2 + m*b^2 = 28*m*b^2

Ug = Ktrans +Krot

4*m*g*b/2 = .5*4*m*v^2 + .5*I*v^2/(-b/2)^2

2*m*g*b = 2*m*v^2 + 2*28*b^2*v^2/b^2
= 2*m*v^2 + 56*m*v^2.

Therefore 29*v^2=g*b.

Therefore v = (g*b/29)^.5;

Is this the correct answer, if not where did I go wrong? Thanks.
I think you have a problem with your moment of inertia and relating the v you calculated to what was asked. If you are treating the two loops as one object and looking for the velocity of the CM, then you need I about the CM. Then you need to recognize that vCM is not the velocity of the center of the big hoop. I doubt that doing neither of these things leads to the correct answer.

You could do separate calculations of energies of the two hoops connecting their velocities at the moment in question by the geometry and solve for v_big, or you can continue to pursue the CM approach you started.
 
I'll try to pursue the cm first and see where it gets me.1st;
Torque = I*(alpha), i.e., 4*m*g*b/2=I*(alpha) => 2*m*g=I*a/b^2, Then I = 2*m*g*b^2/a. So I need another equation with a in it. And such an equation is not obvious to me.
 
John O' Meara said:
I'll try to pursue the cm first and see where it gets me.1st;
Torque = I*(alpha), i.e., 4*m*g*b/2=I*(alpha) => 2*m*g=I*a/b^2, Then I = 2*m*g*b^2/a. So I need another equation with a in it. And such an equation is not obvious to me.
Your energy approach was OK. You can find the moment of inertia about the center of mass using the parallel axis theorem. You just need to know the distance to the CM from a point where you can calculate I. You know how to calculate I for each hoop at its center (that is what you did earlier) so you can find the I for each hoop about the CM of the combination of the two. The net I is just the sum of these two contributions.

http://hyperphysics.phy-astr.gsu.edu/hbase/parax.html
 

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