Finding tension of the string while ball is at top of its path

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To find the tension in the string when the ball is at the top of its vertical path, consider the forces acting on the ball: gravity and centripetal acceleration. At this point, the tension in the string must counteract both the gravitational force and provide the necessary centripetal force to keep the ball moving in a circle. The net force acting on the ball can be expressed as the sum of these forces, with gravity acting downward and the tension acting upward. It's important to understand that in a rotating frame of reference, the centripetal force can be viewed as a fictitious force that feels like a push outward. This conceptual understanding is crucial for solving the problem correctly.
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Homework Statement


A ball on the end of a string is cleverly revolved at a uniform rate in a vertical circle of radius 85.0 cm. If the speed of the ball is 3.25 m/s and its mass is 0.335 kg, calculate the tension in the string when the ball is at the

a) top of its path


Homework Equations



\SigmaFnet force = ma

Fcentripetal = v2/R



The Attempt at a Solution



OK, I have not made an attempt at this problem because my concept of this situation is a little unsure. I don't want any numbers or any calculations, I just want someone to explain to me this problem in just formulas. No numbers at all pleaseeeee
 
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I think you should try it yourself, it's not so hard, at least try. Think of what forces that is exerted upon the ball at the top of the path and in what direction they work.
 
So let me share what I believe it is:

Because the ball is at the top of its path, the forces acting on it include gravity and centripetal acceleration.

If I want to find the tension in the string, then it would be sum of gravity and centripetal acceleration?
 
You're correct about the forces, except with how they interact. When you use a rotating frame of reference for analysis, the centripetal force is replaced by a sort of fictious centrifugal force directed away from the centre.
You can also see it like this: For example: When you travel through a curve in a car, you feel like you are "pushed" outwards toward the edge of the curve. This force which "pushes" you out is fictious and doesn't exist in the real sense, but it still feels like so.

So instead of a centripetal force directed toward the centre at the top, replace it with an equally large opposite facing force
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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