How Do Torque and Force Affect Acceleration and Friction in a Rolling Disc?

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Homework Help Overview

The discussion revolves around the dynamics of a rolling disc subjected to an external force and the effects of torque and friction on its acceleration. The participants are examining the relationships between force, torque, and motion for a disc with specific physical properties, including mass, radius, and moment of inertia.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are attempting to set up equations for torque and force, questioning the correct application of these concepts. They discuss the choice of reference points for calculating torque and the implications of sign conventions in their equations.

Discussion Status

There is an ongoing exploration of different approaches to solving the problem, with some participants providing suggestions and clarifications on the equations to use. The discussion includes varying interpretations of the signs in the equations and the relationships between acceleration and friction.

Contextual Notes

Participants are considering the implications of using different moments of inertia and the conditions under which the parallel axis theorem might apply. There is also a focus on the assumptions regarding the uniformity of the disc and the nature of the forces acting on it.

AdamP
For a disc with mass m, radius R, and moment of inertia about center of mass of (mR^2)/3, and applied external force is F.

A wheel is being pulled by a force F directly upwards, which causes it to roll without slipping (due to static friction), on a horizontal surface. The upward force F is applied at the most right tip or edge of the disc.

Find the acceleration, a, and the static frictional force, f.


I'm not sure how to set up the torque or force equations etc...

So, if F is directly upward, and on the edge, is it like F*cos90=0, so
0-f=ma?
and second equation,
F*(2R)=(moment of inertia about point of contact of disc and surface) * (angular speed)
where
moment of inertia about point of contact = (moment of inertia about center of mass, given) + m*R^2
and
angular speed=a/R (because no slip?)

so in this case, solving the F*2R= --- etc. equation, we get
a=3F/2m
and using 0-f=ma,
f=-3F/2

Does this sound right at all or what should I do? Any suggestion is much appreciated!
 
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Welcome to PF!

AdamP said:
For a disc with mass m, radius R, and moment of inertia about center of mass of (mR^2)/3, and applied external force is F.
Is the disk nonuniform? For a uniform disk [itex]I_{cm} = 1/2 m R^2[/itex].
So, if F is directly upward, and on the edge, is it like F*cos90=0, so
0-f=ma?
The only horizontal force on the disk is the frictional force, so f = ma.
and second equation,
F*(2R)=(moment of inertia about point of contact of disc and surface) * (angular speed)
where
moment of inertia about point of contact = (moment of inertia about center of mass, given) + m*R^2
and
angular speed=a/R (because no slip?)
Both friction (f) and the upward force (F) will exert a torque about the center of mass. Set the net torque equal to [itex]I \alpha[/itex]. (Yes, [itex]a = \alpha R[/itex], since it doesn't slip.)

so in this case, solving the F*2R= --- etc. equation, we get
a=3F/2m
and using 0-f=ma,
f=-3F/2
Redo your solution with my suggestions.
 
Thank you!

So...

Equation 1:
(F-f)*R=I*alpha
(where I is the the moment of inertia going through center of mass, i.e. 1/2mR^2) <--- so we just choose the torque equation to go through the center of mass, is that the easiest case? cos i remember in class we talked about picking the point of contact and use the moment of inertia with respect to that point, like using parallel axis theorem or something... that doesn't apply here does it? on what cases then do we do that?)

Equation 2:
-f=ma=m(r*alpha) <--- do we need the negative sign here? (cos that will affect our result a bit wouldn't it?)

So just solve the two equations two unknowns to get the answer.

(If I used it withOUT the negative sign, I get a=2F/3m, and f=2F/3, does this sound right? the acceleration and friction should be in the opposite directions right, or no..? do we just state it out or what do I do?
cos otherwise, WIth the negative sign, I would have gotten a=-2F/m, and f=-2F, which can't be right... right?)

Thanks!
 
AdamP said:
Equation 1:
(F-f)*R=I*alpha
(where I is the the moment of inertia going through center of mass, i.e. 1/2mR^2) <--- so we just choose the torque equation to go through the center of mass, is that the easiest case? cos i remember in class we talked about picking the point of contact and use the moment of inertia with respect to that point, like using parallel axis theorem or something... that doesn't apply here does it? on what cases then do we do that?)
You can certainly choose the contact point if you like. That makes the equation even easier: [itex]FR = I_{contact} \alpha = 3/2 m R^2 \alpha[/itex].

Equation 2:
-f=ma=m(r*alpha) <--- do we need the negative sign here? (cos that will affect our result a bit wouldn't it?)
The negative sign just depends on your choice of coordinates. I chose positive to be to the left, so both a and [itex]\alpha[/itex] are positive. (Otherwise I can't use [itex]a = I \alpha[/itex].)

So just solve the two equations two unknowns to get the answer.
Right.

(If I used it withOUT the negative sign, I get a=2F/3m, and f=2F/3, does this sound right? the acceleration and friction should be in the opposite directions right, or no..? do we just state it out or what do I do?
These answers look good to me. The acceleration must be in the same direction as the frictional force, since the friction causes the acceleration! (The moral of this story: always draw a careful diagram and identify all the forces and accelerations.)

cos otherwise, WIth the negative sign, I would have gotten a=-2F/m, and f=-2F, which can't be right... right?)
No good. I'll bet you got your signs mixed up somewhere.
 

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