Toboggan on circular arcs

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Physical_Fire
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Hi,
I have a homework question involving conservation of energy and centripetal force. My instructor provided an example with a solution, which I tried to apply to my homework problem, but without success. I tried using V as the initial speed, but in the end I ended up with a range for V. Could someone guide me in the right direction?

Thanks

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kuruman said:
What is the statement of the problem?
What do you mean? The question is attached above.
kuruman said:
Also a diagram would be helpful. What are points A, B and C?
They are symmetrical as far as I can see.
 
kuruman said:
Where do you take the potential energy to be zero?
At the very top; the centre of the circle (D).
 
Physical_Fire said:
At the very top; the centre of the circle (D).
I think that would make thing difficult on the other side of the equation. To begin with, the potential energy at the top of the arc between B and C should negative because the top of the arc is below point D. Secondly, the vertical distance between D and the top of the arc might be a bit tricky to calculate.

I suggest that you choose the potential energy to be zero at the horizontal line from A to C. Then all you have to find is the vertical distance from that line to the top of the arc.

On edit
In the example the zero of potential energy is the centre of the arc on the right at point E in your drawing. You could choose that but then you have to have the vertical distance from E to line AC in order to find the initial potential energy.

WHY?.webp
Also, I think that the solution provided in the example is incorrect. The term ##\cos\theta## does not belong in the ##F=ma## equation provided in the example (see screenshot on the right). It is written when the mass is at the top of the trajectory, where the net force is the weight ##mg## (without the cosine) and the normal force ##R##. The positive direction is assumed "down."
 
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kuruman said:
I suggest that you choose the potential energy to be zero at the horizontal line from A to C. Then all you have to find is the vertical distance from that line to the top of the arc.
Alright. I’ll try doing that but as before I get my answer in terms of V. How do I get in terms of U?
And I think you misread the problem. In the example problem, U is the initial velocity (so mgcos(θ) makes sense) and not the midpoint like in the problem I have to solve.
 
kuruman said:
energy.

WHY?.webp
Also, I think that the solution provided in the example is incorrect. The term cos⁡θ does not belong in the F=ma equation provided in the example (see screenshot on the right). It is written when the mass is at the top of the trajectory, where the net force is the weight mg (without the cosine) and the normal force R. The positive direction is assumed "down."
Correctly, the analysis considers the highest risk of losing contact is at A and B. F=ma is being applied along the normal, so at 45° to the vertical.
 
Physical_Fire said:
I tried using V as the initial speed, but in the end I ended up with a range for V. Could someone guide me in the right direction?
I see no benefit in introducing V. You are to find a range of values for U
First, identify the points of the trajectory which will determine the minimum and maximum speeds and what the constraints are on the speeds at those points. Then use energy conservation to relate those to U.

Physical_Fire said:
At the very top; the centre of the circle (D).
As @kuruman notes, that means the PE at each point will be negative, but you have written them as positive.
 
Physical_Fire said:
Alright. I’ll try doing that but as before I get my answer in terms of V. How do I get in terms of U?
What is in a symbol? If U is the speed at the lowest point of the motion, you are looking for its maximum and minimum values, call them ##U_{\text{max}}## and ##U_{\text{min}}## such that ##U_{\text{min}}<U<U_{\text{max}}.##