How Does Friction Affect the Acceleration of a Rolling Cylinder?

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The discussion revolves around the dynamics of a rolling cylinder subjected to an external force and friction. Participants are exploring how friction influences the linear acceleration of the cylinder's center of mass, with specific focus on torque, forces, and the relationship between linear and angular acceleration.

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Approaches and Questions Raised

  • Participants are attempting to calculate the linear acceleration of the cylinder's center of mass under different conditions, including the presence and absence of friction. They are discussing the application of Newton's laws and the relationship between torque and angular acceleration.

Discussion Status

There are multiple interpretations of the forces and torques acting on the cylinder. Some participants have provided equations relating to the forces and torques, while others are questioning the assumptions made in these equations. The discussion is ongoing, with participants seeking clarification on the relationships between the variables involved.

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Participants are working within the constraints of a homework problem, which may limit the information available for analysis. There is an emphasis on understanding the role of friction and the correct application of physical principles in the context of the problem.

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A rope is wound around a cylinder of mass 4kg and with moment of inertia I=0.020 kg.m^2 about an axis along the cylinder axis, see attachment. If the cylinder rolls without slipping, (a)what is the linear acceleration of its mass center? (b)Repeat for the case where no friction force exists between the table and the cylinder.
So we have a force of 20N applied in the direction shown in the attachment, and the radius of the cylinder is r=10cm.
My attempt: (a)torque T=I*(alpha) where (alpha) is angular acceleration, therefore (alpha)=T/I = 20*.1/.02 = 100rad/s^2
a_tangential=r*(alpha) = 10m/s^2.
a_center=?
(b) F=m*a therefore a_center=20/4=5m/s^2.
Any help would be welcome in redard to what a_center is in part (a). Thanks.
 
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The attachment didn't work. The force of 20N is applied at the top of the rolling cylinder and parallel to the table surface.
 
You have not considered all of the forces acting in part a)
 
Ok I forgot the frictional force f.
20-f=m*a
T-Tf=I*(alpha), where T= torque, Tf =friction torque, alpha= angular acceleration. Now
T-Tf=I*a/r; r*F - r*f = I*a/r therefore
F - f=I*a/r^2 ...(i)
-20 + f=-m*a ...(ii) add i & ii therefore
F-20=I*a/r^2-m*a; => a=20/6=3.333 m/s/s...as F=m*a
a_tangential=3.333m/s^2
a_center=. Can anyone tell me where I might be gone wrong and where?Thanks.
 
John O' Meara said:
Can anyone tell me where I might be gone wrong and where?
There is something wrong with your torque. Look at your free body diagram.
 
Are you saying : T-Tf=I*(alpha) is wrong? which I think you are. Please specify.Thanks. I have got: 20 - f=m*a; T=I*(alpha) and f=(mu)*n ...n=m*g. I have got two unknowns a and f (and really only one independent equation). I must be able to eliminate the frictional force f.
 
John O' Meara said:
Are you saying : T-Tf=I*(alpha) is wrong? which I think you are. Please specify.Thanks. I have got: 20 - f=m*a; T=I*(alpha) and f=(mu)*n ...n=m*g. I have got two unknowns a and f (and really only one independent equation). I must be able to eliminate the frictional force f.
In your equation for ma you have tension and friction acting in opposite directions. Look at where these forces act on the cylinder and the directions. What does that tell you about the torques they produce?
 
I think I have got what you are saying:
20 - f = m*a;
T + Tf =I*(alpha); therefore r*F + r*f = I*a/r and F+f=I*a/r/r; which gives a new equation 20 + F = I*a/r^2 + m*a, now what is F equal to? Is it equal to m*a if it is then a_tangential = 10m/s^2
 
John O' Meara said:
I think I have got what you are saying:
20 - f = m*a;
T + Tf =I*(alpha); therefore r*F + r*f = I*a/r and F+f=I*a/r/r; which gives a new equation 20 + f = I*a/r^2 + m*a, now what is f equal to? Is it equal to m*a if it is then a_tangential = 10m/s^2
Those should be small f in your quote, right? I changed them. This gives you two equations for two unknowns, f and a. f is whatever it has to be to satisfy both equations, as is a.
 
  • #10
20 + f=I*a/r^2 ...(i); 20 - f = m*a ...(ii); a=40/(I/r^2+m) therefore a_tangential = 6.667m/s/s.The question is what is the linear acceleration of the center of the cylinder? The question then is what is the relationship of the linear acceleration to the tangential acceleration. a_tangential = r*(alpha) where (alpha) is the angular acceleration.
 
  • #11
John O' Meara said:
20 + f=I*a/r^2 ...(i); 20 - f = m*a ...(ii); a=40/(I/r^2+m) therefore a_tangential = 6.667m/s/s.The question is what is the linear acceleration of the center of the cylinder? The question then is what is the relationship of the linear acceleration to the tangential acceleration. a_tangential = r*(alpha) where (alpha) is the angular acceleration.
The (a) you defined earlier is the acceleration of the center of the cylinder. You then wrote your angular acceleration in terms of that (a) as alpha = a/r. The tangential acceleration relative to the center of the cylinder is (alpha)*r = = (a/r)*r = a, the same as the acceleration of the center.
 

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