Rolling Ball and angle of incline

AI Thread Summary
A uniform solid sphere rolls down an incline with a linear acceleration of 0.2g, prompting a discussion on calculating the angle of incline using moments of inertia. The moment of inertia for a solid sphere is identified, and the parallel axis theorem is applied to relate forces and angular acceleration. Participants clarify the relationship between linear and angular acceleration, emphasizing that rolling without slipping requires the condition a = αr. Missteps in calculations are addressed, particularly regarding the cancellation of variables. The conversation concludes with a clear distinction that slipping occurs if the equality a = αr is not maintained.
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


\sum \tau = I \alpha
I_{ball} = \frac{2mr^2}{5}

The Attempt at a Solution


Moments about the tipping point:
mgrsin\theta = \frac{2mr^2}{5}\alpha
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,
mgrsin\theta = (\frac{2mr^2}{5} + mr^2)\alpha = \frac{7mr^2}{5}\alpha

Which hardly helps
 
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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)
a_t= \alpha r
 
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frazdaz said:
Like this? (found from one of your posts)
a_t= \alpha r
Yes, exactly.
 
Doc Al said:
Yes, exactly.
I've just never seen that before.

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

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

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:

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

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

No...If a \neq \alpha r ,then slipping occurs .For rolling without slipping a = \alpha r
 
  • #13
frazdaz said:
Does that work as an inequality? i.e. object won't slip providing as long as this holds true a \leq \alpha r
No, it's an equality. If a \ne \alpha r, then there is slipping.
 
  • #14
Doc Al said:
No, it's an equality. If a \ne \alpha r, 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 a \gt \alpha r.

Nonetheless, if you have rolling without slipping, then a = \alpha r.
 
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