You and a friend are going to ride on a Ferris wheel. For a little extra fun, when your friend is at the very top of the Ferris wheel she's going to drop a tennis ball. How far around the Ferris wheel in radians from your friend should you sit so you can catch the ball?
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Hmm, I solved it differently, but anyways, nice solution.
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Post your solution (if you can)...I want to take a look at it.
My Solution: Set the center of the Ferris wheel as the origin. Obviously, x = 4 t , and y = 2 0 − 4 . 9 t 2 . Since the equation of the Ferris Wheel is x 2 + y 2 = 4 0 0 , we can get t 2 ( 2 4 . 0 1 t 2 − 1 8 0 ) = 0 , or t = 2 . 7 3 8 . After plugging this in for the x and y-coordinates, I did some bashing, and I finally found the answer to be 2.0153....
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Bashing Part: The coordinate where the ball intersects the person is (10.952, -16.735). The angle of this point relative to the top of the Ferris Wheel is 2.5618, which means that the person is at an angular distance of 2.5618-2.738*.2= \framebox 2 . 0 1 4 2 from the other person. This solution was more accurate than the last solution, since I used more significant digits for each number.
It is clear that the ball will never reach the bottom of the wheel, since it has a positive velocity at the top:
Using the center of the wheel as the coordinate origin, the path of the ball is
1) Yb = -g x²/(2V²) + 20 where V = R w = 20*0.2 = 4 m/s The wheel height is given by
2) Yw = √[20² - x²]
Equating (1) & (2) → x = 10.952 m
Thus, the intersection angle below horizontal Θi = arccos[10.952/20] = 0.9913 rad, and
Total angle Θ = (π/2) + Θi = 2.562 rad
Time for the ball to fall to the intersection point t = √[2y/g] where y = 20(1+sinΘi) = 36.734 m →t = 2.7385 sec
The angle your friend travels through during this time is Θf = w t = 0.2 2.7385 = 0.5477 rad
So, the angle your friend should sit in front of you ß = Θ - Θf = 2.014 rad
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From the diagram, it is clear that,
y = 2 1 g t 2
x = R ω t
⇒ y = 2 R 2 ω 2 g x 2
Now, let us the find the point of intersection of this parabolic path of the ball, with the circle (Ferris wheel), whose equation is :
x 2 + ( y − R ) 2 = R 2
Substituting y = 2 R 2 ω 2 g x 2 in the equation of the circle, we get,
x 2 ≈ 1 2 0 m
⇒ x = 1 2 0 m
⇒ y = 3 6 . 7 5 m
Now, to find the angle θ , we shall take the dot product of ( x i ^ + y j ^ ) − R j ^ and the vertical unit vector j ^ .
Thus,
( x i ^ + ( y − R ) j ^ ) ⋅ j ^ = x 2 + ( y − R ) 2 cos θ
Putting the values of x , y , R , we get,
cos θ = 8 0 − 6 7
⇒ θ = 2 . 5 6 3 r a d
Now, considering the catcher of the ball,
θ = θ o + ω t
We already have θ , thus, to find θ o , we just need to find t , which we will derive from the fact that,
x = R ω t
⇒ t = 2 . 7 3 8 s e c
Substituting the values of θ , ω , t , we get,
θ o = 2 . 0 1 5 r a d is the final answer.