adjacent said:
I don't know about momentum and functions and Centripetal force equation all that yet; I am in 9th grade
No problem, it's not that hard as long as we stick with the simple case: We have a weight tied to the end of a string, we're spinning it about our head, we won't worry about gravity pulling the weight down, and we can change the radius by pulling in on the string to reduce the radius or letting the string out to increase the radius, and only consider the situation when the weight is moving in a perfect circle (it may do some funny stuff while the radius is actually changing), the string has no mass and doesn't stretch.
In this ideal case, the tension in the string (this is the centripetal force) will be
[tex]F=\frac{mv^2}{r}[/tex]
where m is the mass, v is its speed, and r is the radius of the circle. This can be calculated from Newton's second law (or you can take my word for it)
The quantity called angular momentum is given (in this simplified case only, but that's good enough here) by [itex]L=mvr[/itex] and it will remain constant as we pull the string in or let it out, causing both v and r to change. This is "The Law of Conservation of Angular Momentum".
You know the initial radius and speed so you can calculate the initial value of L and F, and you can use the angular momentum formula to see how the speed changes with the radius (remember, L cannot change in this setup unless you deliberately spin the thing faster), and then the force formula to see how the force changes.