Kinda hard problem involving friction and a spool.

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SUMMARY

The discussion centers on calculating the critical angle θc at which a spool transitions from rolling to skidding under the influence of a tension T applied at an angle θ. The correct expression for θc is derived as θc = cos⁻¹(r/R), where r is the inner radius and R is the outer radius of the spool. Participants clarify that the torque due to tension is τ = Tr, and the torque due to static friction is τ = f_sR. The relationship between these torques and the forces acting on the spool is essential for determining the conditions for rolling versus skidding.

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  • #31
schaefera said:
My bad I apologize! But how do we solve the case with linear acceleration since we can't use the same algebra to cancel everything we don't know?

In case of skidding, the friction is kinetic, instead of being static. You know that kinetic friction is μN. You can express N with the weight and T and the angle.

There are two equations, one for linear acceleration, and the other for angular acceleration. You can solve both in terms of tension, angle, mass and moment of inertia and see how they are related at different pulling angles.

ehild
 
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  • #32
So, the case where it's static friction is the one case in which there is no acceleration and then we turn the cranks with kinetic friction there to find forward and backwards dependencies?
 
  • #33
schaefera said:
So, the case where it's static friction is the one case in which there is no acceleration and then we turn the cranks with kinetic friction there to find forward and backwards dependencies?

No, there is static friction in case of pure rolling. During rolling, there can be acceleration, both linear and angular, related by the equation a=R dω/dt.
The rolling can happen both forward and backwards.

When the spool skids, the friction is kinetic. There can be both linear and angular acceleration.

ehild.
 
  • #34
ehild said:
No, there is static friction in case of pure rolling. During rolling, there can be acceleration, both linear and angular, related by the equation a=R dω/dt.
The rolling can happen both forward and backwards.

When the spool skids, the friction is kinetic. There can be both linear and angular acceleration.

ehild.

We're asked when the spool switches from rolling to skidding. So rolling with skidding shouldn't be considered...
 
  • #35
calculate the critical value of θ (call it θc) at which the condition goes from rolling to skidding.

It is not the spool that switches from rolling to skidding.
Applying the same tension, the spool will not switch from rolling to skidding at the critical angle, but from rolling to standing...
But it can skid at the critical angle without rotating.

Do you only want to answer to the problem writer? Are you not interested in the phenomenon?

ehild
 
  • #36
See next post whoops
 
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  • #37
Right, so another way to think of this:

If the frictional force is kinetic, then by definition it opposes the motion of the object, meaning the object must be skidding to the right.

If friction is static, then the tension has not yet pulled hard enough on the object to overcome the static frictional force to the left, meaning that the object will roll, but to the left (there wasn't enough force to cause it to accelerate right). Think of this as if you're pulling on the string, but the static friction is so strong that it causes the object to pivot (and begin to spin) toward the left.

Now clearly, as long as it's moving to the right, it's can't roll smoothly (that is, roll without skidding) because the tension to the right is stronger than the kinetic friction to the left... but if the tension is causing a torque that makes it want to rotate counter-clockwise, this will be stronger than the friction wanting it to rotate clockwise. Thus, w has a negative value while v has a positive value, so we can never meet the wR=v condition for smooth rolling.

Thus, the critical angle is the angle where the skidding to the right would switch to rolling to the left!
 
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  • #38
ehild said:
It is not the spool that switches from rolling to skidding.

Umm...what changes from rolling to skidding/standing, if not the spool? :confused:

But it can skid at the critical angle without rotating.

This is what I'm trying to say. :smile:

Do you only want to answer to the problem writer? Are you not interested in the phenomenon?

ehild

Very much so. I enjoy scientific phenomena much more than school-questions. But this being a homework thread, I guess charmedbeauty must be looking for a way to solve his problem o:)

Would be really interesting to discuss this in the General science sub-forums!

schaefera said:
If the frictional force is kinetic, then by definition it opposes the motion of the object, meaning the object must be skidding to the right.

If friction is static, then the tension has not yet pulled hard enough on the object to overcome the static frictional force to the left, meaning that the object will roll, but to the left. Think of this as if you're pulling on the string, but the static friction is so strong that it causes the object to pivot (and begin to spin) toward the left.

Thus, the critical angle is the angle where the skidding to the right would switch to rolling to the left!

Yep. That's how I think it is, too. At angles above the critical, you will have the spool moving backwards, and angles below the critical, it will move forward.
 
  • #39
It's a little hard to get into that mindset, because it almost sounds like it's asking when it begins to roll after it has already been sliding to the right... clearly, that can't happen though, which I didn't realize until I pictured it that way!
 
  • #40
Hi, Charmedbeauty,
we almost forgot about you...

charmedbeauty said:
ohh I think I get it from the eqn above solve for fs

fs=ma+Tcosθ
Correct.
charmedbeauty said:
s=ma+Tcosθ

That equation is valid at the limiting case when the spool starts to skip...

charmedbeauty said:
torque=fsR-Tr=ma

The torque is equal to angular acceleration times moment of inertia: βI

In case of pure rolling, the spool moves with velocity V and rolls with angular velocity ω=V/R. A similar relation is valid between the linear acceleration of the spool and the angular acceleration of its rotation: a=Rβ. So you can write the torque equation in the form

fsR-Tr=Ia/R.

From this equation and from the one you wrote for the acceleration,

fs=ma+Tcosθ

you can cancel fs and find the acceleration of the rolling spool. If you have the formula for a, you can discuss it: at what angles does the spool accelerate forward or backward, and which is the angle where the angular acceleration is zero so rolling can not start.
Substituting the acceleration back into the first equation for fs, you can check if fs is not greater than the maximum static friction μsN.


ehild
 

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