Minimum Speed for Steel Ball on Inclined Loop-the-Loop

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The discussion centers on determining the minimum speed a steel ball must have at the top of a loop-the-loop to remain on the track. It emphasizes the importance of centripetal force, which is necessary for maintaining circular motion. The key insight is that at the top of the loop, the gravitational force (mg) must equal the required centripetal force for the ball to stay in contact with the track. By setting the normal force to zero, the minimum speed is derived as v = square root of (gR). This conclusion clarifies the relationship between speed, gravitational force, and the forces acting on the ball at the top of the loop.
endeavor
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A steel ball rolls down an incline into a loop-the-loop of radius R. What is the minimum speed the ball must have at the top of the loop in order to stay on the track? (the ball has a radius r and starts at a height of h)
This is a similar image to the one in my book:
http://img98.imageshack.us/img98/1876/1m40209ji.th.jpg

I'm not sure how to solve this question. But I think it has something to do with conservation of energy. I tried doing that and got:
v = square root of (v02 - 20/7 gR)
but the answer is the square root of (gR), which is must simpler than my answer...so I must be doing something wrong.
 
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It has to do with centripetal force, rather than energy conservation.
The ball has to not fall off the top of the track, which means it must maintain a minimum amount of circular motion.
It is centripetal force that provides this circular motion.
When traveling around a track, it is the normal reaction of the track against the ball which provides the centripetal force.
When the motion is in a vertical plane, this reaction is modified by any radial component of the ball's weight.
At the top of the track, the radial component of the ball's weight is mg.
If there is no reaction force from the track then mg is the minimum amount of centriptal force.
If mg maintains circular motion (no falling off the top of the track) then mg = mw²r
 
Fermat said:
If there is no reaction force from the track then mg is the minimum amount of centriptal force.
This 2nd last sentence I don't understand.
 
There are two forces acting on the ball at the top of the loop: gravity and the normal force (the track pushing on the ball). These forces add to produce the centripetal force on the ball. The faster the ball goes, the greater will be the normal force. To find the minimum speed such that the ball barely maintains contact with the track, set that normal force to zero. (Then apply Newton's 2nd law.)
 
I think I'm beginning to understand.
But why does the normal force have to be greater if the speed is greater? Is it because there needs to be a greater force to keep the ball in the loop? (Rather than fly off tangentially)

so I use Fcentripetal = mg, and get the answer v = square root of (gR)
 
endeavor said:
Is it because there needs to be a greater force to keep the ball in the loop? (Rather than fly off tangentially)
Exactly.

so I use Fcentripetal = mg, and get the answer v = square root of (gR)
Right.
 
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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