Rotating ring on a rough surface- but with a twist

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SUMMARY

The discussion focuses on the mechanics of a ring with two attached masses (m and 2m) rolling on a rough surface. Participants analyze the center of mass (com) of the ring, which is calculated to be at R/5, and explore the implications for angular acceleration, frictional force, and normal reaction. Key equations such as torque (τ = Iα) and the parallel axis theorem are emphasized for solving the problem. The conversation highlights the importance of drawing free body diagrams (FBD) to visualize forces acting on the system.

PREREQUISITES
  • Understanding of rotational dynamics and torque (τ = Iα)
  • Familiarity with the parallel axis theorem for moment of inertia calculations
  • Ability to calculate center of mass for composite systems
  • Knowledge of free body diagram (FBD) construction for analyzing forces
NEXT STEPS
  • Study the application of the parallel axis theorem in complex systems
  • Learn how to derive angular acceleration in rolling motion scenarios
  • Investigate the role of friction in rolling objects on rough surfaces
  • Practice drawing and analyzing free body diagrams for various mechanical systems
USEFUL FOR

Students and educators in physics, particularly those focusing on mechanics, as well as engineers and anyone involved in analyzing dynamic systems involving rotational motion.

  • #61
Lnewqban said:
... and to the imbalance of masses around the ring: that is the driving torque.

If you take your point of view as the center of the ring, you will see the ring pushing the surface rearward.
In order to do that, the ring needs "to be able to grab" onto the surface.
I have a question: if I look at ANY point on the ring relative to some other point, will it be in circular motion? Or is this true only relative to the geometric center of the ring and IAOR?
 
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  • #62
palaphys said:
. . . the center of mass is the geometric center, it just goes in a straight line right?.
Wrong. The center of the ring follows a straight line because it is always at distance ##R## above ground. The distance of the CM above ground varies from ##R+\frac{1}{5}R## at its highest to ##R-\frac{1}{5}R## at its lowest.
 
  • #63
kuruman said:
Wrong. The center of the ring follows a straight line because it is always at distance ##R## above ground. The distance of the CM above ground varies from ##R+\frac{1}{5}## at its highest to ##R-\frac{1}{5}## at its lowest.
I meant in a general case, not this case. Here the center of mass follows a circular path relative to the geometric center?
 
  • #64
erobz said:
If you would draw a FBD you should be able to see that if the wheel is accelerating to the right, there is some force acting to the right. What force can act to the right? Which way is normal force. Which, direction are the weight forces, is anyone pushing the wheel etc... are questions you should be asking yourself. At the very least by process of elimination you should see that there must be a horizontal force, and where it must act.
Only the center of the wheel is accelerating right. Correct? The center of mass of the wheel has a tangential accn, centripetal acceleration, and the acceleration of the center of the ring. Please correct me if wrong
 

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  • #65
palaphys said:
But will friction not cause angular retardation if it acts towards the right? Then how will the no slip condition be maintained?
Is there a moment arm of ##f## about the instantaneous center of rotation?
 
  • #66

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  • #67
erobz said:
Is there a moment arm of ##f## about the instantaneous center of rotation?
No, but there is a moment arm about the center of the ring right.. the IAOR is always at rest momentarily?
 
  • #68
palaphys said:
Only the center of the wheel is accelerating right. Correct? The center of mass of the wheel has a tangential accn, centripetal acceleration, and the acceleration of the center of the ring. Please correct me if wrong
Mark the center of mass on a diagram. Next let system it roll without slipping to the point where the ##2m## mass is directly below the center of the ring and the ##m## mass directly above it. Can you conclude whether the center of mass has changed position?
 
  • #69
erobz said:
Mark the center of mass on a diagram. Next let system it roll without slipping to the point where the ##2m## mass is directly below the center of the ring and the ##m## mass directly above it. Can you conclude whether the center of mass has changed position?
Yes I can. It is going in circular motion right.. with radius r÷5 if u see from center of ring
 
  • #70
palaphys said:
Yes I can. It is going in circular motion right.. with radius r÷5 if u see from center of ring
Well how did it change position if it didn't accelerate?
 
  • #71
erobz said:
Well how did it change position if it didn't accelerate?
It has tangential and centripetal accl? Combined with accl of geometric center like this maybe?
 

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  • #72
palaphys said:
Only the center of the wheel is accelerating right. Correct?
You said this. It makes me believe that you believe the center of mass is not accelerating to the right initially as well?
 
  • #73
erobz said:
You said this. It makes me believe that you believe the center of mass is not accelerating to the right initially as well?
I wanted to say that the geometric center of the wheel is just accelerating in a straight line sorry for confusion
 
  • #74
erobz said:
You said this. It makes me believe that you believe the center of mass is not accelerating to the right initially as well?
Please tell me how the tendency to slip is towards the left.. I still can't believe it.. please
 
  • #75
palaphys said:
I wanted to say that the geometric center of the wheel is just accelerating in a straight line sorry for confusion
Well, I'm trying to get you to see that if the center of mass (not explicitly the center of the wheel) there must be a force acting on the body ( via Newton's Second) that accelerates the center of mass as it moves in this case.
 
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  • #76
erobz said:
Well, I'm trying to get you to see that if the center of mass (not explicitly the center of the wheel) there must be a force acting on the body ( via Newton's Second) that accelerates the center of mass as it moves in this case.
I see that .. just can't predict what direction friction is going to be. It seems intuitive that it would be towards right, but I want a physics proof why it is so.
 
  • #77
palaphys said:
I see that .. just can't predict what direction friction is going to be. It seems intuitive that it would be towards right, but I want a physics proof why it is so.
In this case the wheel is initially pushing on the ground to the left, and the ground is pushing the wheel to the right...via friction. This thing is just a pendulum whose pivot moves back and forth. The wheel will have some oscillatory motion, first it goes to the right then it turns back and heads to the left. friction flips with acceleration. Its observer to be "accelerationally" dependent. If you assume it, and correctly carry out the mathematics, the math will tell you. Here its observationally obvious, in other problems it might be challenging to get it out of the gate.
 
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  • #78
palaphys said:
I have a question: if I look at ANY point on the ring relative to some other point, will it be in circular motion? Or is this true only relative to the geometric center of the ring and IAOR?
All points of the ring instantaneously rotate about the instantaneous ring-surface point of contact, which is constantly disappearing while another contact point, located just a little further, is constantly assuming the function of a new instantaneous pivot, around which all the points of the ring rotate again, and so on.

The succession of those points of contact moves horizontally at the same velocity of the geometrical center of the rolling ring, keeping always apart from each other the same vertical distance, which equals the radius of the ring.
 
  • #79
I think I've figured out the normal reaction part. Please check my work someone.
 

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  • #80
Lnewqban said:
The succession of those points of contact moves horizontally at the same velocity of the geometrical center of the rolling ring, keeping always apart from each other the same vertical distance, which equals the radius of the ring.
I don't understand this part please make it simple
 
  • #81
erobz said:
In this case the wheel is initially pushing on the ground to the left, and the ground is pushing the wheel to the right...via friction. This thing is just a pendulum whose pivot moves back and forth. The wheel will have some oscillatory motion, first it goes to the right then it turns back and heads to the left. friction flips
I am extremely confused with friction in this case. What i was taught was that friction opposes relative tendency of motion. Here all of you are saying something else. Generally how I found direction of friction in rolling type of questions was by assuming none at all, and observing tendency of slipping. Please explain in simpler way pls
 
  • #82
Could someone please verify this
 

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  • #83
palaphys said:
I am extremely confused with friction in this case. What i was taught was that friction opposes relative tendency of motion. Here all of you are saying something else. Generally how I found direction of friction in rolling type of questions was by assuming none at all, and observing tendency of slipping. Please explain in simpler way pls
You are confusing kinetic friction with static friction. Kinetic friction is molecules sliding past each other, breaking structure permanently - converting mechanical energy to internal energy, and static friction is armwrestling with a wall...you might be warping it a bit, but it's springing back. Thats as far as I can see in plain terms.
 
  • #84
palaphys said:
@kuruman hope this is right
It is correct.
 
  • #85
erobz said:
You are confusing kinetic friction with static friction. Kinetic friction is molecules sliding past each other, breaking structure, and static friction is armwrestling with a wall...you might be warping it a bit, but it's springing back.
That's not my confusion. I know that it's static friction here. The direction of friction is spoiling my day. I'm not able to figure it out.
 
  • #86
kuruman said:
It is correct.
How about this
 

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  • #87
palaphys said:
I see that .. just can't predict what direction friction is going to be. It seems intuitive that it would be towards right, but I want a physics proof why it is so.
You don't need a proof, just logic. For the CM to accelerate to the right there must be a horizontal force acting on it. How many forces are there that act in the horizontal direction on any of the masses here?
 
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  • #88
kuruman said:
You don't need a proof, just logic. For the CM to accelerate to the right there must be a horizontal force acting on it. How many forces are there that act in the horizontal direction on any of the masses here?
How is the CM accelerating to the right? You said it was a cycloid path right? Also check the screenshot I posted.how can I conclude that it is horizontal?
 
  • #89
palaphys said:
That's not my confusion. I know that it's static friction here. The direction of friction is spoiling my day. I'm not able to figure it out.
But you are confused about it. You said you were taught friction always opposes motion. It doesn't, I'm trying to clarify that concept for you. There are two distinct names, two concepts to grapple with. One of them (static friction) is a fickle mistress.
 
  • #90
erobz said:
But you are confused about it. You said you were taught friction always opposes motion. It doesn't, I'm trying to clarify that concept for you. There are two distinct names, two concepts to grapple with.
friction does not oppose relative motion?
 

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