Vertical Circular Motion Problem

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Homework Help Overview

The discussion revolves around a vertical circular motion problem involving forces acting on a block and a stone. Participants explore the dynamics of centripetal force, weight, and normal force at different positions in the circular path.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants attempt to analyze the forces at the top and bottom of the circular motion, questioning the roles of weight and normal force. Some explore the concept of pseudo forces and their implications on the forces acting on the box and stone.

Discussion Status

The discussion is ongoing, with participants raising questions about the direction and magnitude of forces involved. There is a focus on clarifying the relationship between normal force and weight, as well as the implications of constant versus varying speed in the context of the problem.

Contextual Notes

Some participants express confusion regarding the assumptions of constant speed and the nature of the forces acting on the system. The problem does not specify external forces, leading to varied interpretations of the forces at play.

Mickey Tee
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Homework Statement


Circular Motion.PNG

Homework Equations


Centripetal Acceleration = v2/r
Fnet = ΣF

The Attempt at a Solution


The block exerts a force W equal to its weight on the box at the top most position.
This upward W minus W downwards and an unknown F downwards equals a net Fc downwards. So F equals Fc

At the bottom position there is a W downwards and the total force on the box is this W plus something else
The net force is Fc upwards since the speed is constant

Now I get completely confused.
 
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Mickey Tee said:

Homework Statement


View attachment 76215

Homework Equations


Centripetal Acceleration = v2/r
Fnet = ΣF

The Attempt at a Solution


The block exerts a force W equal to its weight on the box at the top most position.This upward W minus W downwards and an unknown F downwards equals a net Fc downwards. So F equals Fc

What is the direction of the force the stone applies at the box? What is the force the box exerts on the stone? So what is your unknown force?
Mickey Tee said:
At the bottom position there is a W downwards and the total force on the box is this W plus something else
The net force is Fc upwards since the speed is constant

Now I get completely confused.
That "something else " is the normal force from the block, the block exerts on the stone.
 
What if I think in terms of pseudo force? The pseudo force at the top position is the centripetal force upwards, so the force exerted by the stone on the box is
Fc - mg = mg
=> Fc = 2mg

At the bottom position, pseudo force is downwards, along with mg. So the force by the stone on the box is 3mg. But the answer is 7mg :(
 
Mickey Tee said:
What if I think in terms of pseudo force? The pseudo force at the top position is the centripetal force upwards, so the force exerted by the stone on the box is
Fc - mg = mg
=> Fc = 2mg

At the bottom position, pseudo force is downwards, along with mg. So the force by the stone on the box is 3mg. But the answer is 7mg :(
You make yourself confused with the pseudo force. It is not the centripetal force. Use inertial frame of reference. The stone moves together with the box along a circle. It needs the appropriate centripetal force. The centripetal force is the resultant of two forces, what are they at the top of the circle?
 
I think at the top its (mg - N). But isn't there also an mg downwards? And isn't the normal force self adjusting?

Um, can you tell me how the normal force varies as the box goes around the circle?
 
Mickey Tee said:
isn't the normal force self adjusting?
Yes, it adjusts as necessary to keep the stone moving in the circle - as long as that does not involve its going negative.
ehild said:
The centripetal force is the resultant of two forces, what are they at the top of the circle?

Mickey Tee said:
I think at the top its (mg - N)
You think the resultant is that?
Mickey Tee said:
But isn't there also an mg downwards?
I think you may be getting confused by the happenstance that the normal force equals mg here. Set that aside for the moment and just label it N. Which way does N act at the top? Which way does the weight mg act at the top?
 
Mickey Tee said:
I think at the top its (mg - N). But isn't there also an mg downwards? And isn't the normal force self adjusting?
The picture shows the box touching the stone on the upper side. The box can only push the stone, in what direction? Up or down?
 
You're not told that there are external forces acting on the circle. In addition to what has been already said, it can be helpful to think about it in terms of a conserved quantity.

I don't see a reason to assume that the velocity is constant as the problem says.
 
The normal force would be 3mg in case of constant speed. If case of conservation of energy, the normal force would be 7mg.
 

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