A boy, a cart, a loop , an icecream-cone

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In summary, the conversation revolved around a problem of finding the radius R of a loop in order for a boy to reach his falling ice cream cone at the bottom of the loop at the same time he reaches the bottom of the hill. The solution involved using conservation of energy and finding the time it takes for the boy to slide down the loop. However, this requires an elliptic integral and may need some approximations.
  • #1
Nebuchadnezza
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Was sitting in class thinking about this problem, did some rough sketches of a solution but never really managed to solve it.

![Ice cream cone and a loop-de-loop][1]

D8XAh.png


Question:
Assume a boy starts at the top of a circle with radius [itex]R[/itex] as described in the picture. It is a snowy day and the path can be considered frictionless. The boy enters a loop with radius [itex]r[/itex] at the bottom of the hill. At the top of the loop the boy loses his icecream cone in such a way that it starts falling. The initial velocity of the ice-cream is [itex]0[/itex] m/s straight down.

The problem is to find [itex]R[/itex] expressed by [itex]r[/itex], such that the boy reaches the ice-cream just as he reaches the bottom of the loop​


The problem boiled down to finding out how much time the boy uses getting from the top of the loop to the bottom. Any help, solutions or inputs would be great.

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My attempt, I know that this is most likely 90% wrong

By using conservation of mechanical energy. The speed at the bottom of the hill equals

[tex] v_b^2 = Rmg [/tex]

And the velocity at the top of the loop equals

[tex] v_t^2 = 2g\left( R - 2r \right) [/tex]

Vi know that the aceleration is constant and equals [itex] g [/itex] (Here is where I think I make my mistake, forgot to account for the angular velocity)

[tex] s = \dfrac{v_1 - v_0}{2} t [/tex]

We use this equation to find out how long it takes the boy to get from the top, to the bottom of the loop.

[tex] t \, = \, \dfrac{2s}{v_1 - v_0} \, = \, \dfrac{2\left( \dfrac{2\pi r}{2}\right)}{\sqrt{2gR} - \sqrt{2g(R - 2r)}} [/tex]

Now we figure out how long it takes the icream to fall the distance of the diameter or [itex] 2r [/itex] .

[tex] s = v_0 + \dfrac{1}{2}gt^2 [/tex]
[tex] t = \sqrt{\dfrac{2s}{g}} \, = \, \sqrt{\dfrac{4r}{g}} \, = \, 2 \sqrt{\dfrac{r}{g}} [/tex]

By setting these two equations equal each other, and solving for [itex] R [/itex] , we obtain that

[tex] R = \dfrac{16+8 \pi^2+\pi^4) r}{8 \pi^2} \cdot r \approx 2.43 r [/tex]

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Any comments, suggestions, hints soloutions would be much obliged =)
 
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  • #2
The time for the boy to slide down the semicircle is found from integrating the conservation of energy formula. It is however an elliptic integral so you'd have to make an approximation somewhere.
 
  • #3
Could you elaborate a bit more, would one turn the loop sideways. And integrate with respect to r?
 

1. What is the purpose of the cart in the scenario?

The cart serves as a mode of transportation for the boy and his ice cream cone.

2. Where is the loop located in relation to the boy and the cart?

The loop is not mentioned in the scenario, so it is unclear where it is located.

3. What flavor is the ice cream cone?

The flavor of the ice cream cone is not specified in the scenario.

4. Why is the boy carrying an ice cream cone?

The scenario does not provide a reason for why the boy is carrying an ice cream cone.

5. What could happen if the cart hits the loop?

Since the loop is not mentioned in the scenario, it is unknown what could happen if the cart were to hit it.

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