Rolling Ball and angle of incline

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Homework Help Overview

The problem involves a uniform solid sphere and a thin spherical shell rolling down an incline without slipping. The goal is to determine the angle of the incline based on the linear acceleration of the center of mass.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the relationship between linear and angular acceleration, the application of moments of inertia, and the use of the parallel axis theorem. There are questions about the implications of the equations derived and the conditions for rolling without slipping.

Discussion Status

The discussion is ongoing, with participants exploring various aspects of the problem, including the correct application of equations and the conditions necessary for rolling without slipping. Some guidance has been offered regarding the relationships between different types of acceleration.

Contextual Notes

Participants are considering the implications of their calculations and the assumptions made regarding the conditions of motion, including the role of friction and the setup of the problem.

frazdaz
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Homework Statement



A uniform solid sphere rolls down an incline without slipping. If the
linear acceleration of the centre of mass of the sphere is 0.2g, then what
is the angle the incline makes with the horizontal? Repeat for a thin
spherical shell.

Homework Equations


[tex]\sum \tau = I \alpha[/tex]
[tex]I_{ball} = \frac{2mr^2}{5}[/tex]

The Attempt at a Solution


Moments about the tipping point:
[tex]mgrsin\theta = \frac{2mr^2}{5}\alpha[/tex]
Don't think this is going anywhere but I can't think of any other way to include moments of inertia.

Just thought, this moment of inertia is from the centre of the ball, not the tipping point. Correct?

So, by the parallel axis theorem,
[tex]mgrsin\theta = (\frac{2mr^2}{5} + mr^2)\alpha = \frac{7mr^2}{5}\alpha[/tex]

Which hardly helps
 
Last edited:
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So far, so good. Now relate the linear acceleration of the center of mass to the angular acceleration.
 
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Doc Al said:
So far, so good. Now relate the linear acceleration of the center of mass to the angular acceleration.
Like this? (found from one of your posts)
[tex]a_t= \alpha r[/tex]
 
Last edited:
frazdaz said:
Like this? (found from one of your posts)
[tex]a_t= \alpha r[/tex]
Yes, exactly.
 
Doc Al said:
Yes, exactly.
I've just never seen that before.

[tex]mgrsin\theta = \frac{7mr^2}{5} \frac{g}{5}[/tex]
[tex]sin\theta = \frac{7r}{25}[/tex]
Does it want it in terms of r or have I gone wrong?
[tex]\theta = sin^{-1}(\frac{7r}{25})[/tex]
 
frazdaz said:
I've just never seen that before.

[tex]mgrsin\theta = \frac{7mr^2}{5} \frac{g}{5}[/tex]
[tex]sin\theta = \frac{7r}{25}[/tex]
Does it want it in terms of r or have I gone wrong?
[tex]\theta = sin^{-1}(\frac{7r}{25})[/tex]

Recheck your calculations.You have missed an 'r' while making substitution. 'r' will cancel out .
 
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Tanya Sharma said:
Recheck your calculations.You have missed an 'r' while making substitution. 'r' will cancel out .
Ahhh, of course. Thank you!
I take it the tangential acceleration is in the direction of the linear velocity? And is the radial acceleration just the centripetal acceleration?
 
frazdaz said:
Ahhh, of course. Thank you!
I take it the tangential acceleration is in the direction of the linear velocity? And is the radial acceleration just the centripetal acceleration?

Tangential acceleration and radial acceleration of what ? In this problem we are dealing with linear and angular acceleration of the sphere.
 
frazdaz said:
I've just never seen that before.
That's the condition for 'rolling without slipping'.
 
  • #10
frazdaz said:
Ahhh, of course. Thank you!
I take it the tangential acceleration is in the direction of the linear velocity? And is the radial acceleration just the centripetal acceleration?
The condition for rolling without slipping relates the linear acceleration of the center of mass to the angular acceleration:

[tex]a = \alpha r[/tex]
 
  • #11
Doc Al said:
The condition for rolling without slipping relates the linear acceleration of the center of mass to the angular acceleration:

[tex]a = \alpha r[/tex]
Does that work as an inequality? i.e. object won't slip providing as long as this holds true [tex]a \leq \alpha r[/tex]
 
  • #12
frazdaz said:
Does that work as an inequality? i.e. object won't slip providing as long as this holds true [tex]a \leq \alpha r[/tex]

No...If [itex]a \neq \alpha r[/itex] ,then slipping occurs .For rolling without slipping [itex]a = \alpha r[/itex]
 
  • #13
frazdaz said:
Does that work as an inequality? i.e. object won't slip providing as long as this holds true [tex]a \leq \alpha r[/tex]
No, it's an equality. If [itex]a \ne \alpha r[/itex], then there is slipping.
 
  • #14
Doc Al said:
No, it's an equality. If [itex]a \ne \alpha r[/itex], then there is slipping.
How would it slip if the linear acceleration smaller than the RHS? I can picture the ball accelerating so quickly that it begins to slip, but not the other way around.
 
  • #15
frazdaz said:
How would it slip if the linear acceleration smaller than the RHS? I can picture the ball accelerating so quickly that it begins to slip, but not the other way around.
Imagine the ball spinning, without enough traction.

In practice, if you were to start the ball from rest at the top of the incline and there were insufficient friction to prevent slipping, you would have [itex]a \gt \alpha r[/itex].

Nonetheless, if you have rolling without slipping, then [itex]a = \alpha r[/itex].
 
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