How Does Slipping Affect the Acceleration of a Rolling Ball?

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SUMMARY

The discussion focuses on the dynamics of a rigid ball with mass 6 kg and radius 0.23 m subjected to two forces: 55 N to the right and 20 N to the left. The coefficient of friction between the ball and the table is 0.435. The calculations yield an angular acceleration of 34.2 rad/s² and a normal force of 58.8 N, while the friction force is determined to be -12.2 N, indicating that the ball experiences slipping. The key issue raised is the discrepancy between the calculated friction force and the expected static friction force, μN.

PREREQUISITES
  • Understanding of rigid body dynamics and acceleration point relations.
  • Familiarity with Newton's laws of motion, particularly ƩF=ma and ƩM=Iα.
  • Knowledge of the moment of inertia and radius of gyration, specifically I=mk².
  • Concept of static versus kinetic friction and conditions for rolling without slipping.
NEXT STEPS
  • Study the implications of slipping in rigid body dynamics, focusing on the transition from static to kinetic friction.
  • Learn about the conditions for rolling without slipping and how to apply them in practical scenarios.
  • Explore the effects of varying coefficients of friction on the motion of rigid bodies.
  • Investigate the relationship between angular acceleration and linear acceleration in rolling objects.
USEFUL FOR

Students of physics, mechanical engineers, and anyone involved in the study of dynamics and motion of rigid bodies will benefit from this discussion.

CaptainP
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Homework Statement


A rigid ball of mass m = 6kg and radius R = .23 m is sitting on a table. The mass center and geometric center of the ball coincide, but the radius of gyration about its mass center is k = .19 m. The ball is initially at rest. There is a coefficient of friction μ = .435 between the ball and the table. Two forces are then applied to the ball: a force F1 = 55 N to the right at the center of mass, and a force F2 = 20 N to the left at the very top of the ball. Given this, determine the angular acceleration of the ball and the linear acceleration of the ball's center at the instant the forces are first applied.


Homework Equations


I=mk^2 where k is the radius of gyration.
Acceleration point relation for rigid bodies
ƩF=ma
ƩM=Iα

The Attempt at a Solution


The acceleration at the point of contact must be zero. Because the ball is initially at rest, this means that the acceleration at the center of the ball is simply αR because the ball is a rigid body. Assume that the friction force f, which acts at the point of contact, points to the left.

Next, we use Newton's law in the x and y directions. This gives F1 - F2 - f = ma = mrα and N - mg = 0. Then we take the sum of the moments about the center of the ball, which yields F2R - fR = mk2α. Without making the assumption that f = μN, we solve these three equations for 3 unknowns to find that N = 58.8 Newtons, f = -12.2 Newtons and α = 34.2 rad/s2.

This is where I get lost, because clearly f≠μN. How do I reconcile this? What assumptions am I making that are incorrect?
 
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CaptainP said:

Homework Statement


A rigid ball of mass m = 6kg and radius R = .23 m is sitting on a table. The mass center and geometric center of the ball coincide, but the radius of gyration about its mass center is k = .19 m. The ball is initially at rest. There is a coefficient of friction μ = .435 between the ball and the table. Two forces are then applied to the ball: a force F1 = 55 N to the right at the center of mass, and a force F2 = 20 N to the left at the very top of the ball. Given this, determine the angular acceleration of the ball and the linear acceleration of the ball's center at the instant the forces are first applied.


Homework Equations


I=mk^2 where k is the radius of gyration.
Acceleration point relation for rigid bodies
ƩF=ma
ƩM=Iα

The Attempt at a Solution


The acceleration at the point of contact must be zero.

The title of your thread is "rolling ball with slipping" If the ball slips, the point of contact accelerates, and the rolling condition aCM=αR does not hold.

CaptainP said:
Because the ball is initially at rest, this means that the acceleration at the center of the ball is simply αR because the ball is a rigid body. Assume that the friction force f, which acts at the point of contact, points to the left.

Next, we use Newton's law in the x and y directions. This gives F1 - F2 - f = ma = mrα and N - mg = 0. Then we take the sum of the moments about the center of the ball, which yields F2R - fR = mk2α. Without making the assumption that f = μN, we solve these three equations for 3 unknowns to find that N = 58.8 Newtons, f = -12.2 Newtons and α = 34.2 rad/s2.

This is where I get lost, because clearly f≠μN. How do I reconcile this? What assumptions am I making that are incorrect?

You determined the angular acceleration and force of static friction of the rolling ball, that does not slip. Is the static friction equal to μN?


ehild
 

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