Find angle of the sphere losing contact with the surface

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Homework Help Overview

The problem involves a solid sphere rolling down a hemisphere and seeks to determine the angle at which the sphere loses contact with the surface. The context includes considerations of forces, energy conservation, and the dynamics of rolling motion.

Discussion Character

  • Exploratory, Assumption checking, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the calculations leading to an angle of 54°, with some questioning the assumptions made regarding the size of the sphere relative to the hemisphere. Others suggest that practical observations yield different results, indicating potential discrepancies between theoretical predictions and experimental outcomes.

Discussion Status

The discussion is ongoing, with participants exploring various interpretations of the problem. Some have provided insights into the role of friction and the conditions under which the sphere may slip before losing contact. There is a recognition of differing experimental results, prompting further inquiry into the measurements and assumptions involved.

Contextual Notes

Participants note that the problem may involve approximations, particularly when considering the size of the sphere relative to the hemisphere. There are also mentions of measurement techniques and the accuracy of the experimental setup, which may influence the observed angle at which the sphere loses contact.

Adriano25
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Homework Statement


A solid sphere rolls down a hemisphere from rest. Find the angle at which the sphere loses contact with the surface.
R = radius of hemisphere
a = radius of sphere

Homework Equations


ΣFr = Macm,r
N-mgcosθ = -mVcm2/(R+a)
N = mgcosθ - mvcm2/(R+a) eq. (1)

Conservation in mechanical energy
mg(R+a) = 1/2mvcm2 + 1/2Icmω2 + mg(R+a)cosθ
mg(R+a) = 1/2mvcm2 + 1/2(2/5ma2)(Vcm/a)2 + mg(R+a)cosθ
mg(R+a) = 7/10mVcm2 + mg(R+a)cosθ
Simplified
7/10mVcm2 + mg(R+a)(1-cosθ)
Vcm2 = 10g/7 (R+a)(1-cosθ) eq. (2)

eq. (2) into eq. (1)
N = mgcosθ - m10g(R+a)/(R+a) (1-cosθ)
N= 17mgcos/7 - 10mg/7
N goes to 0 since the sphere loses contact with the surface, thus:
0 = 17cosθ-10
θ = cos-1(10/17)
θ = 54°

The Attempt at a Solution



My attempt solution has been trying to prove this problem experimentally. By rolling a solid sphere on a hemisphere, the angle I found was much smaller than 54°. Any thoughts?
 
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Adriano25 said:

Homework Statement


A solid sphere rolls down a hemisphere from rest. Find the angle at which the sphere loses contact with the surface.
R = radius of hemisphere
a = radius of sphere

I found some notes on this problem and that looks like the right answer. Although, that is for a small ball where ##a << R##.

I can't follow your working, but you must have made that approximation somewhere.

PS I think it's the same answer for any ##a##.

Also, as rolling without slipping requires a minimum amount of friction to accelerate, the sphere is bound to slip before it comes off. In practice, therefore, it will start to slip and gain higher speed earlier, so come off earlier.
 
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Thus, the sphere would start slipping right before it comes off? I can't seem to notice that. Also, would it be possible to do a calculation to find a better and more approximate angle?
 
Adriano25 said:
Thus, the sphere would start slipping right before it comes off? I can't seem to notice that. Also, would it be possible to do a calculation to find a better and more approximate angle?
You could redo the calculation assuming no friction, so no rotation. That at least would give you a range for the angle.
In between, you would have to work in terms of forces and torques rather than energy.

What angles are you observing? How are you measuring them?
 
I'm observing an angle approximately half of the angle I measured per my calculations. I'm just measuring it by observation. I'm still very confused in why the experiment is not working as desired and how I could get a better approximation.
 
Adriano25 said:
I'm observing an angle approximately half of the angle I measured per my calculations. I'm just measuring it by observation. I'm still very confused in why the experiment is not working as desired and how I could get a better approximation.
So you are seeing it become airborne when only about a third of the way around the arc?
 
haruspex said:
So you are seeing it become airborne when only about a third of the way around the arc?
Yes. I was expecting it to come off at around 45 degrees.
 
Adriano25 said:
Yes. I was expecting it to come off at around 45 degrees.
But you calculated 54 from vertical, no?
What are you using for the hemisphere? How accurately shaped?
 
Yes, from the vertical. I'm using a big Earth sphere pretty accurate.
 
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Adriano25 said:
Yes, from the vertical. I'm using a big Earth sphere pretty accurate.
Then I'm out of ideas. Even a sliding point particle should stay on until about 48 degrees.
 

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