Finding the time for an object to start rolling without slipping

In summary, the time it takes for an object to start rolling without slipping is determined by analyzing the forces and torques acting on it. The key factors include the object's mass, radius, frictional force, and the moment of inertia. By applying Newton's second law and the rotational equivalent, one can derive an equation that relates these variables, ultimately allowing for the calculation of the time required for the object to transition from sliding to rolling motion.
  • #1
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Homework Statement
I am trying to derive the equation that my textbook presents (5.28), however, I notice that they don't use the right hand rule for the torque so there is a slight change in the sign in my derivation
Relevant Equations
##v_r = r\omega## for is a condition for rolling without slipping where ##v_r## is the speed of the COM of the object
For this,
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I don't understand why they don't have a negative sign as the torque to the friction should be negative. To my understanding, I think the equation 5.27 should be ##I\frac{d \omega}{dt} = -F_{friction}R## from the right hand rule assuming out of the page is positive.

Noting that ##f_k = \mu_kmg## and integrating both sides, I get the equation of motion ##\frac{-Rmg \mu_kt}{I} = \omega(t)##

I also get ##v(t) = v_0 - u_kgt##

So setting the two equations equal to each other in the relation for rolling motion:

##v(t) = R \omega (t) ##

I get ##t_r = \frac{v_0}{\mu_kg(1 - \frac{mR^2}{I})}##. Could someone please explain to me who is wrong and why?

Many thanks!
 
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  • #2
ChiralSuperfields said:
assuming out of the page is positive.
What you quote of the problem does not indicate whether the motion is left to right or right to left. Assuming usual conventions and a positive velocity, it is L to R. In that case, the angular acceleration is clockwise, so negative and into the page.
Correspondingly, at rolling, ##v=-R\omega##.
 
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  • #3
haruspex said:
What you quote of the problem does not indicate whether the motion is left to right or right to left. Assuming usual conventions and a positive velocity, it is L to R. In that case, the angular acceleration is clockwise, so negative and into the page.
Correspondingly, at rolling, ##v=-R\omega##.
Thank you for your reply @haruspex! However, do you please know where the equation ##v = -R \omega## came from? Sorry I have not seen that equation with the minus sign before (I have only seen ##v = R \omega##)

Many thanks!
 
  • #4
ChiralSuperfields said:
Thank you for your reply @haruspex! However, do you please know where the equation ##v = -R \omega## came from? Sorry I have not seen that equation with the minus sign before (I have only seen ##v = R \omega##)

Many thanks!
The commonest convention is positive to the right for velocity and positive anticlockwise for rotation. If a disc is rolling to the right along a line underneath it then its rotation is clockwise, so a positive velocity means a negative rotation, etc.
You can think of it as being because the radius, measured from the axis to the ground contact is downwards, so negative. If it were rolling along the ceiling then there would be no minus sign.
 
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  • #5
haruspex said:
The commonest convention is positive to the right for velocity and positive anticlockwise for rotation. If a disc is rolling to the right along a line underneath it then its rotation is clockwise, so a positive velocity means a negative rotation, etc.
You can think of it as being because the radius, measured from the axis to the ground contact is downwards, so negative. If it were rolling along the ceiling then there would be no minus sign.
Thank you for your help @haruspex! Your explanation makes sense
 

FAQ: Finding the time for an object to start rolling without slipping

What conditions must be met for an object to start rolling without slipping?

For an object to start rolling without slipping, the static friction between the object and the surface must be sufficient to prevent relative motion. This means that the force of static friction must be greater than or equal to the force causing the object to slide. Additionally, the object's rotational inertia and the torque applied must be balanced so that the object begins to roll rather than slide.

How do you calculate the time it takes for an object to start rolling without slipping?

The time it takes for an object to start rolling without slipping can be calculated using the equations of motion for both linear and rotational dynamics. By setting the linear acceleration equal to the tangential acceleration (a = r*α, where r is the radius and α is the angular acceleration), and solving for the time, you can determine when the conditions for rolling without slipping are met.

What role does static friction play in rolling without slipping?

Static friction is crucial for rolling without slipping as it provides the necessary force to initiate rotational motion. Without sufficient static friction, the object would slide rather than roll. Static friction ensures that the point of contact between the object and the surface does not move relative to the surface, allowing the object to roll smoothly.

How does mass distribution affect the time for rolling without slipping?

The mass distribution of an object affects its moment of inertia, which in turn impacts the angular acceleration. Objects with a higher moment of inertia will take longer to start rolling without slipping because they require more torque to achieve the same angular acceleration. Conversely, objects with a lower moment of inertia will start rolling more quickly under the same conditions.

Can rolling without slipping occur on any surface?

Rolling without slipping can occur on any surface as long as the static friction is sufficient to prevent slipping. This means that the surface must provide enough resistance to match the force causing the motion. On very smooth or slippery surfaces, it may be difficult or impossible for an object to roll without slipping due to inadequate static friction.

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