Rolling with slipping and conditions for not slipping

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SUMMARY

The discussion focuses on the conditions for rolling without slipping of a wheel with radius R, emphasizing the relationship between linear velocity (v), angular velocity (ω), and static friction. The condition for rolling without slipping is established as v = ωR, contingent upon sufficient static friction to ensure the contact point remains stationary. The conversation highlights the importance of understanding the forces and moments acting on the wheel, as well as the role of friction during angular acceleration. Key insights include the necessity of calculating required frictional force and the implications of insufficient friction on the wheel's motion.

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  • Understanding of rotational dynamics and kinematics
  • Familiarity with static and dynamic friction coefficients
  • Knowledge of Newton's laws of motion
  • Basic principles of torque and angular acceleration
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  • Study the effects of static and dynamic friction on rolling motion
  • Learn about the equations of motion for rotating bodies
  • Explore experimental setups to measure rolling friction
  • Investigate the relationship between torque and angular acceleration in various scenarios
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cromata
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Suppose that we have a some rotating object (lets say a wheel with radius R). Let's observe this problem from some reference frame in which center of mass translates with some velocity v and rotates with angular velocity ω. I know that condition for rolling without slipping is v=ωR (point at which wheel touches ground doesn't move). Also, I know that is only possible if coefficient of static friction is large enough so that point that touches ground has velocity 0.
But I don't really understand how to determine if the friction is large enough to cause rolling without slipping: how does it depend on the angular velocity of the wheel (or some other parameters)?
 
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Once the object is rolling, and obeying the equation you gave, the friction becomes irrelevant. In an ideal frictionless setup it would continue moving as if it were rolling even if the surface became frictionless. Imagine a flywheel rolling along a carpet and then going off the end of the carpet onto ice. Conservation of momentum and angular momentum would dictate that nothing changes.

Where friction is important is when there is angular acceleration. This is viscerally plain when a vehicle skids when too much acceleration is applied (think drag cars doing burnouts) or it brakes too hard. The angular velocity of the wheel plays no part in the calculation.
 
cromata said:
But I don't really understand how to determine if the friction is large enough to cause rolling without slipping: how does it depend on the angular velocity of the wheel (or some other parameters)?

some simple experiments can be designed to study and understand the stages of rolling and the limiting conditions for rolling.

the following study may help you to see the role of rolling friction and it can be measured using a theoretical analysis as well-

ref.- https://billiards.colostate.edu/physics/Domenech_AJP_87%20article.pdf
 
cromata said:
But I don't really understand how to determine if the friction is large enough to cause rolling without slipping: how does it depend on the angular velocity of the wheel (or some other parameters)?
You have to know all other forces and moments acting on the wheel. Then you can combine the force and moment equations via v=ωR (or its time derivative a=αR), and solve for the required frictional force. If its magnitude is less than the normal force time static friction coefficient, it will roll. Otherwise it will slide, so you use dynamic friction coefficient to get the friction force and work out a and α from that.
 
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A.T. said:
You have to know all other forces and moments acting on the wheel. Then you can combine the force and moment equations via v=ωR (or its time derivative a=αR), and solve for the required frictional force. If its magnitude is less than the normal force time static friction coefficient, it will roll. Otherwise it will slide, so you use dynamic friction coefficient to get the friction force and work out a and α from that.
Let's assume that there is some external force creating torque on the wheel, but it doesn`t affect translation (it`s possible if the force is in vertical direction in our wheel example). If coefficient of static friction is not large enough for rolling without slipping, will then wheel translate with constant acceleration N*k/m? (where k is coefficient of friction)?
 
cromata said:
Let's assume that there is some external force creating torque on the wheel, but it doesn`t affect translation (it`s possible if the force is in vertical direction in our wheel example). If coefficient of static friction is not large enough for rolling without slipping, will then wheel translate with constant acceleration N*k/m? (where k is coefficient of friction)?

As has already been pointed out, friction is only necessary for acceleration. Once the wheel is rotating, no friction is required for it to continue rotating. Moreover, there is no minimum static friction needed. Although, the less friction you have, the less acceleration you can get.
 
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cromata said:
Let's assume that there is some external force creating torque on the wheel, but it doesn`t affect translation (it`s possible if the force is in vertical direction in our wheel example). If coefficient of static friction is not large enough for rolling without slipping, will then wheel translate with constant acceleration N*k/m? (where k is coefficient of friction)?
Yes, assuming k is the coefficient of dynamic friction and no other horizontal forces are acting.
 
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Thank you for your answers
 

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