Little confusion regarding centripetal force in vertical circle

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Discussion Overview

The discussion revolves around the dynamics of a mass in vertical circular motion, specifically focusing on the forces acting on a pendulum at the topmost point of its swing. Participants explore the relationship between gravitational force, tension in the string, and centripetal force, while addressing common confusions regarding these concepts.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant describes the forces acting on a mass at the top of a vertical circle, noting that both gravitational force and tension act downwards, leading to confusion about how the mass does not fall.
  • Another participant argues that minimum tension does not imply slack in the string, clarifying that some tension is necessary to maintain the circular motion.
  • There is a discussion about the role of gravitational force at the top of the circle, with one participant suggesting that the component of gravitational force keeping the string taut is zero at that point.
  • Some participants mention that if the mass reaches the top with non-zero speed, it can continue moving even if the tension becomes zero, leading to further questions about the nature of the forces involved.
  • One participant states that the sum of tension and weight equals the centripetal force, emphasizing that centripetal force is a resultant force that produces centripetal acceleration.
  • A participant provides equations for the minimum velocity required at the top and bottom of the circle to maintain circular motion without falling off.

Areas of Agreement / Disagreement

Participants express varying interpretations of the role of tension and gravitational force at the top of the circle. There is no consensus on whether the string becomes slack or how the forces interact, indicating ongoing disagreement and confusion.

Contextual Notes

Some participants highlight the importance of energy conservation and the conditions under which the mass can complete a circular motion, but these aspects remain unresolved and depend on specific assumptions about the system.

exuberant.me
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consider a pendulum. The mass 'm' is hung and now we are interested in finding the velocity so that it completes one circle. Clearly we can do it easily by conserving energy.

Now my problem is with the top most point.
Clearly the tension is minimum at this point so that string becomes slack.
The forces acting on the mass is mg downwards, Tension downwards
and since its in circular motion so the centripetal force acts towards the center.
"How then does the particle not fall", is what my confusion is.
since all the forces are downwards.
However, i know this is completely untrue. The centripetal force equals mg + T acting on the mass but what about the "direction" it should act in outward direction but as i have read and know that centripetal force acts towards the center. Clear it please.
Thanks in advance!
 
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Minimum tension does not mean the string becomes slack. That would require zero tension (or perhaps coming up with a negative value of tension, which is impossible, when solving a problem). Minimum tension does not have to be zero, and the string does not become slack as long as there is some tension.

You're correct that the net force must be downward when the object is at the top of the circle.
 
oooo yes i got it
that means its just the component of mg that keeps the string tight and at the top most point this component of mg is 0 right...!
Thank u!
 
hi exuberant.me! :smile:
exuberant.me said:
Clearly the tension is minimum at this point so that string becomes slack.
The forces acting on the mass is mg downwards, Tension downwards
and since its in circular motion so the centripetal force acts towards the center.
"How then does the particle not fall", is what my confusion is.
since all the forces are downwards.

yes, the only force is downward, and therefore the acceleration is downward

(vector) acceleration is rate of change of (vector) velocity, so the velocity downward-component is increasing (from zero) …

but the velocity sideways-component stays the same, so the velocity becomes slightly sloping downward, not 100% downward :wink:

however, the above reasoning is irrelevant, since (if there is exactly enough energy to just reach the vertical) the string actually becomes slack before it reaches the vertical :redface:
 
But where does this outward velocity come from??
Is it imaginary or what is it that keeps the string straight and not slack?
 
sorry … i wasn't clear :redface:

if the mass reaches the top with non-zero speed, then it will keep going even if the tension is zero (which however you could only achieve by shortening the string)

in fact the mass won't reach the top (if the string stays the same length) because it will have started following a parabola (with slack string) earlier
 
exuberant.me said:
oooo yes i got it
that means its just the component of mg that keeps the string tight and at the top most point this component of mg is 0 right...!
Thank u!
Not sure I understand your question here. The force of gravity is always mg, directed downward. And mg can't be zero, ever, so long as m is not zero.
:confused:
 
exuberant.me said:
The forces acting on the mass is mg downwards, Tension downwards
and since its in circular motion so the centripetal force acts towards the center.
"How then does the particle not fall", is what my confusion is.
since all the forces are downwards.

The sum of tension an weight IS the centripetal force.
There is no third force.
"Centripetal" is called any force or force resultant which produces the centripetal acceleration.
 
Velocity at top of the circle must be at least

vt = √(gR)

R is the radius of the circle.

To make a complete circle without falling off the top, velocity at the bottom of the circle must be at least

vb = √(5gR).

Another way to look at it is

vb = √(5) * vt

All these you can find from centripetal force and conservation of energy.
 

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