Softball in vertical circle, find release velocity

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SUMMARY

The problem involves calculating the release velocity of a 0.236 kg softball that is pitched in a vertical circular path with a radius of 0.633 m. The initial speed at the top of the circle is 12.8 m/s, and a 30 N force is exerted parallel to the motion. The correct approach requires incorporating the work done by the 30 N force into the energy equations, as energy is not conserved due to this external force. The final velocity upon release can be determined using the equation vf = √(vi² + 4gr + (2 * Work)/m), where Work is the work done by the external force.

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  • Understanding of kinetic and potential energy equations (K = 1/2mv², U = mgh)
  • Familiarity with the work-energy theorem
  • Basic principles of circular motion
  • Ability to manipulate algebraic equations
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  • Study the work-energy theorem in detail, focusing on its application in non-conservative systems.
  • Learn about forces acting on objects in circular motion, particularly the role of tension and external forces.
  • Explore energy conservation principles in systems with external work applied.
  • Practice solving problems involving circular motion and external forces to build confidence.
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AHinkle
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Homework Statement


A softball pitcher rotates a 0.236 kg ball
around a vertical circular path of radius
0.633 m before releasing it. The pitcher exerts
a 30 N force directed parallel to the motion
of the ball around the complete circular path.
The speed of the ball at the top of the circle
is 12.8 m/s.
The acceleration of gravity is 9.8 m/s2 .
If the ball is released at the bottom of the
circle, what is its speed upon release?
Answer in units of m/s.


Homework Equations


K = 1/2mv2
Ki+Ui=Kf+Uf ?Maybe

The Attempt at a Solution


I believe this is flawed but here's what I tried to do...

r = 0.633meters

Kf = (1/2)mvf2
Ki = (1/2)mvi2
Uf = mgh where h=0 (I set the reference point at the bottom of the circle i.e.
hbottom=0) I believe this is okay because it's only the change in potential energy we're after
Ui=mg(2r) (i used to 2r because if the bottom is 0 then the diameter (2r) is the height above 0)

(1/2)mvf2=(1/2)mvi2+2mgr
(I did not include Uf because h is 0 at the bottom so the whole quantity goes to zero)

mvf2 = 2((1/2)mvi2 + 2mgr)
mvf2 = mvi2+4mgr
m(vf2) = m(vi2+4gr)
(the masses cancel)

vf2 = vi2+4gr

vf=(vi2+4gr)1/2

vf=((12.8)2+4(9.8)(0.633))1/2

vf=13.7351 m/s

This was needless to say, not the correct answer.
Reasons why I think I failed:
1) They gave a force in the question. The model I used was for an isolated system (i.e. no influence from outside agents) is the 30N force from an outside agent? or is the pitcher's hand part of the system?
2) Maybe the work-kinetic energy theorem doesn't work in a circle? I am good with things in a straight line. Circles throw me.

Please help, thanks
 
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AHinkle said:
.
.
.

Homework Equations


K = 1/2mv2
Ki+Ui=Kf+Uf ?Maybe
.
.
.
vf=13.7351 m/s

This was needless to say, not the correct answer.
Reasons why I think I failed:
1) They gave a force in the question. The model I used was for an isolated system (i.e. no influence from outside agents) is the 30N force from an outside agent? or is the pitcher's hand part of the system?
2) Maybe the work-kinetic energy theorem doesn't work in a circle? I am good with things in a straight line. Circles throw me.

Please help, thanks
Your intuition is correct about why the approach you used didn't work out. The 30N force comes into play here.

The 30 N force is doing work on the ball, so that will add to the ball's energy. So instead of the ball's energy being conserved, we have
Ef = Ei + [work done on ball by 30 N force]​

If you can figure out the "work done..." part of the equation, it should work out. E is K+U, of course.
 

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