What is the force on the ball's lowest point in a vertical revolving motion?

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In a discussion about the forces acting on a ball in vertical circular motion, participants analyze the forces at the highest and lowest points of the motion. The ball, with a mass of 20 grams, experiences a tension of 0.2 Newtons at the top, leading to a calculated force of 1.4 Newtons at the bottom. Key points include the need to account for different speeds at the top and bottom due to conservation of energy, and the correct application of centripetal force concepts. Participants also clarify the conversion between kinetic energy and centripetal force, ultimately arriving at a tension value close to the expected result. The conversation emphasizes the importance of understanding the dynamics of circular motion and energy conservation principles.
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Hello there!

My study mate and I have been trying to figure this one out but have not had success. This is the problem we would appreciate to get some help with:

A ball with mass of 20 grams is attached to a robe and is revolving vertikal in a circle. There is no energy beeing added to it. At the ball highest point, a force of 0.2 Newton is pulling on the robe. What is the force on the ball"s lowest point?

The statet result says 1.4 Newton.

The most logical way of solving this problem is that at the highest point, the sum of all forces is the the centripedal force minus the gravitational force:

0.2 N = - mg + m\omega^2r

At its lowest, the sum of the forces that act on the ball should be
F = + mg + m\omega^2r

Is this assumption right? With those to equations we get 0.4 Newton, which sounds actually good to me. Maybe my professor is wrong ?!

Any help will be appreciated!
 
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Your method looks OK to me - but using that same method I don't get 0.4N

Use the first eqn to find a value for mw^2 rAlthough neither do I get 1.4N - any suggestions anyone?
 
fara0815 said:
The most logical way of solving this problem is that at the highest point, the sum of all forces is the the centripedal force minus the gravitational force:

0.2 N = - mg + m\omega^2r

At its lowest, the sum of the forces that act on the ball should be
F = + mg + m\omega^2r
Two comments:
(1) You assume the same angular speed at top and bottom. Not so: At the bottom, the ball will be going faster. (Remember conservation of energy.)

(2) "centripetal force" is not a force! It's a term used to describe the net force acting towards the center in circular motion. So, the net force on the ball at the top is:
F_{net} = -T -mg

This equals the "centripetal force", via Newton's 2nd law applied to circular motion:
F_{net} = - m v^2/r

So:
-T -mg = - m v^2/r

Where I take down to be negative. At the bottom, the tension and acceleration both point up. (And the speed and tension are different, of course.)
 
Hmm, When we do this at A-level we always have the stone traveling at constant speed.

is it posible to solve this otherwise, with no further info?
 
Sure you can solve it: Use conservation of energy.
 
Yes, but when I tried that, I was left with r in the equation, which we don't have.

What have I missed?

...I'll keep trying...
 
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Cancel that, think I've got rid of the r and yes, it gives the answer required.

fara, from the top of the circle, when you find a value for mv^2/r, you have to be able to convert this to kinetic energy. The at the bottom, after you've added the KE gained, you have to be able to convert it back to a new value of mv^2/r

Unless there's a quicker way, Dr Al?
 
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thank you very much guys for your help but unfortunately, I am totally clueless about converting the \frac{mv^2}{r} into kinetic energy. It just does not appear to me ! :(
 
(mv^2)/r and 0.5 mv^2

So to convert mv^2/r to KE you multiply by r/2

Use the data you've been given for the top pf the circle to find mv^2/r
Convert it to ke.

Add on the ke you gain (from GPE) from top to bottom of circle.

Now you have the total ke at the bottom. This time, to turn it back to mv^2/r you multiply by 2/r - handy because otherwise you´d be left with an r in the expression.

Now use your original T = mg + mv^2/r at the bottom to find the tension.

I got 1.38 doing it this way - which is close enough to what you want.
 
  • #10
yeah! I have got 1.377 N but I do not understand why you can multiply it by \frac{r}{2} to have it converted into KE.
Here is what I figured out:

Situation 1, top :
-T_1-mg=-ma_1
Situation 2, bottom:
T_2-mg=ma_2

Thus
a_1=g+\frac{T_1}{m}=w^2_1r
a_2=\frac{T_2}{m}-g=w^2_2r

So with that I get the velocities:
V^2_1=(g+\frac{T_1}{m})r
V^2_2=(\frac{T_2}{m}-g)r

Conservation of Energy says:

KE+KP=KE
\frac{1}{2}mV^2_1+mg2r=\frac{1}{2}mV^2_2

After solving it to T_2 I got:
2gm+T_1+4gm=T_2
and that is 1.37 N!

We really appreciate your help guys!
 
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  • #11
hurrah!

as for the conversion, well they both contain mv^2 , one divided by 2 and one divided by r. So you use the r and the 2 to convert one to the other.
 
  • #12
well, sometimes it is so obvious that one cannot see it ;)
 
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