High School Explain FBD in vertical circle

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SUMMARY

The discussion centers on the forces acting on a pebble moving in a vertical circle, specifically addressing the balance of weight and tension. It is established that while tension provides the necessary centripetal force, the weight of the pebble does not need to be balanced at all points in the motion, particularly when the string is horizontal. The conversation highlights that the motion is not uniform circular motion due to the presence of tangential acceleration, which varies the speed of the pebble as it moves through the vertical circle. The conclusion drawn is that vertical uniform circular motion is theoretically impossible, while horizontal uniform circular motion can be achieved.

PREREQUISITES
  • Understanding of Newton's laws of motion, particularly Newton's 2nd law.
  • Knowledge of centripetal force and its role in circular motion.
  • Familiarity with concepts of kinetic and potential energy in the context of circular motion.
  • Basic grasp of tangential and radial acceleration in physics.
NEXT STEPS
  • Study the principles of centripetal force in detail, focusing on its calculation and application.
  • Learn about the conservation of energy in circular motion, including kinetic and potential energy transformations.
  • Explore the differences between uniform and non-uniform circular motion, with practical examples.
  • Investigate the dynamics of horizontal circular motion and the forces involved, including tension and weight components.
USEFUL FOR

Physics students, educators, and anyone interested in understanding the dynamics of circular motion, particularly in vertical and horizontal contexts.

Deepak verma
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Hi ,

just curious about the F.B.D of a pebble moving in a vertical circle, which component that balances the weight of the pebble at the horizontal position , as tension is providing the required centripetal force , weight is acting downwards , which component balances it ?
 
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Why do you think the weight needs to be balanced?
 
it has to be , otherwise system won't be working as it does . There is no counter force to balance it. a system is in equilibrium has all ∑force = 0 .
 
Deepak verma said:
it has to be , otherwise system won't be working as it does . There is no counter force to balance it. a system is in equilibrium has all ∑force = 0 .
The system is not in equilibrium.
 
not in equilibrium but forces should be balanced as it is a case of uniform circular motion no tangential acceleration only centripetal .
[Mentor's note: This post has been edited to remove some unnecessary personal argumentation]
 
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Deepak verma said:
not in equilibrium but forces should be balanced as it is a case of uniform circular motion no tangential acceleration only centripetal .
Even in uniform circular motion the forces are not balanced; the object is accelerating in some direction and this requires some non-zero net force.
 
Deepak verma said:
not in equilibrium but forces should be balanced as it is a case of uniform circular motion no tangential acceleration only centripetal .
But motion in a vertical circle (such as a rock tied to a rope, spun in a circle) is not uniform circular motion. There will be a tangential acceleration.

As Nugatory already pointed out, for accelerated motion (which this is an example of) the forces aren't "balanced" but comply with Newton's 2nd law.
 
@Nugatory , I understand there should be some net force but that force is centripetal force acting towards center not the weight , weight has to be balanced as it has no tangential acceleration.

My main concern is at a particular point that is when string is horizontal weight simply acts downwards and as no counter component is there it should not complete the circle because acceleration g is acting downwards.
 
Deepak verma said:
@Nugatory
My main concern is at a particular point that is when string is horizontal weight simply acts downwards and as no counter component is there it should not complete the circle because acceleration g is acting downwards.
What is the tension in the string at that moment? What is the acceleration of the weight at that moment?

The situation might be a bit easier to visualize if you imagine the object to be moving along a circular track instead of the end of a stretched string.
 
  • #10
Tension would be equal to centripetal force and acceleration is towards the center v sqaure divided by radius of circle . See everything is defined except weight component.
 
  • #11
Deepak verma said:
Tension would be equal to centripetal force and acceleration is towards the center v sqaure divided by radius of circle . See everything is defined except weight component.
And the weight is defined too; in fact, it's the only force in the problem which is constant in both magnitude and direction.

You're mistaken about the direction of the acceleration; there are only two points in the circle where the tangential component of the acceleration is zero, and they aren't where the string is horizontal.
 
  • #12
Deepak verma said:
@Nugatory , I understand there should be some net force but that force is centripetal force acting towards center not the weight , weight has to be balanced as it has no tangential acceleration.

My main concern is at a particular point that is when string is horizontal weight simply acts downwards and as no counter component is there it should not complete the circle because acceleration g is acting downwards.
What point of the trajectory are you referring to? Top, bottom, on the side?
 
  • #13
Side.
 
  • #14
If it is a uniform circular motion , then there won't be any tangential acceleration throughout the motion , I'm talking theoretically not practically , I know there is no motion as uniform circular motion but still my doubt persist. Weight at other position counter balance tension or provide tension and centripetal force not at horizontal position that is my concern
 
  • #15
On the horizontal position of the string the weight is tangential so there is tangential acceleration. The tension is radial so there is centripetal acceleration.
This motion is not uniform, not even theoretically. The speed changes as the body moves along the circular trajectory. It has a maximum speed at the bottom point and a minimum speed at the top point. There is no point on the trajectory where the forces are balanced.
If the forces are balanced (net force equal to zero) the only motion possible is in a straight line, with constant speed.
 
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  • #16
Deepak verma said:
If it is a uniform circular motion , then there won't be any tangential acceleration throughout the motion , I'm talking theoretically not practically , I know there is no motion as uniform circular motion but still my doubt persist. Weight at other position counter balance tension or provide tension and centripetal force not at horizontal position that is my concern
You've specified motion in a vertical circle, so it isn't uniform circular motion.

Conservation of energy requires that the sum of the kinetic energy and the potential energy of the weight be constant; but the potential energy is greater at the top of the circle than at the bottom, so the kinetic energy and hence the speed must therefore be less at the top than at the bottom. More informally, the speed must change because gravity is slowing the weight on the upswing and speeding it up on the downswing. The speed can only change if there is a tangential component to the acceleration; it does change, so therefore there must be a tangential component to the acceleration.
 
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  • #17
@thank you nasu , i got the point . thank you everyone .
 
  • #18
And one more thing , so I can conclude , there is no vertical uniform circular motion theoretically as well. But horizontally it would be possible right?
 
  • #19
Deepak verma said:
And one more thing , so I can conclude , there is no vertical uniform circular motion theoretically as well. But horizontally it would be possible right?
Sure. And using the same example -- the rock on a rope, but now spun horizontally -- the weight of the rock would be balanced by the tension in the rope. The rope would not be horizontal, but at an angle.
 
  • #20
yeah in that case :

Tcosθ = mg and , Tsinθ= mv(square)/r
 
  • #21
Right.
 

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