Calculating Tension, Moment of Inertia, and Angular Speed in a Rotating System

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The discussion focuses on solving a physics problem involving a mass attached to a cord wrapped around a wheel, requiring calculations of tension, moment of inertia, and angular speed. Participants emphasize the importance of correctly drawing free body diagrams (FBDs) to identify real forces acting on the system, such as tension, gravity, and normal force. Clarifications are made regarding the distinction between real forces and the concept of force derived from acceleration (m*a), which is not a force itself. The correct approach involves using equations of motion to find tension and subsequently calculate the moment of inertia and angular speed. Ultimately, the original poster successfully applies the equations and arrives at the correct answers with guidance.
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An m = 12.4kg mass is attached to a cord that is wrapped around a wheel of radius r = 10.0cm (see the figure below). The acceleration of the mass down the frictionless incline is measured to be a = 2.10m/s^2.
a) Assuming the axle of the wheel to be frictionless, and the angle to be θ = 36.2deg determine the tension in the rope.
b) Determine the moment of inertia of the wheel
c)Determine angular speed of the wheel 2.04s after it begins rotating, starting from rest.

All in all I just have a lot of trouble drawing free body diagrams and just figuring out how to approach a problem with my given set of known variables.

On my initial attempt for part a) I tried drawing a free body diagram but I didn't know if I should add the value I get from mgsin(theta) to the value that I got for F (I used m*a to get that value).

I've uploaded my attempt at a solution and I didn't get very far. I feel like there's a process at solving these questions but I just don't get it. Any help would be appreciated.

RoughWork.jpg
Inertia Image.png
 
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Why do you think that there is a force F? It is not mentioned in the problem statement.

I think you are a victim of Mr. d'Alembert!

Draw your FBDs with on the forces (the actual forces, not those you imagine) acting on the bodies. Then sum forces and set Sum F = m*a.
 
Dr.D said:
Why do you think that there is a force F? It is not mentioned in the problem statement.

I think you are a victim of Mr. d'Alembert!

Draw your FBDs with on the forces (the actual forces, not those you imagine) acting on the bodies. Then sum forces and set Sum F = m*a.

So there is no force at all acting on the block? If they give you an acceleration and a mass, wouldn't the product of those two be the force heading down the ramp? That's something that confuses me in FBDs. When is there actually a force present? When one is being constantly applied by an external object only?
 
No one said that there are no forces on the block. It is pretty clear that there are forces (1) normal to the ramp and acting on the block, ( 2) a force (tension) in the cord. If friction were involved, this would be yet another force. Oh, and don't forget the force of gravity (the weight). All of these are real forces; m*a is NEVER a force.

Read what Newton's law says: Sum F = m*a
All of the (real) forces go on the left side.
 
One more thing: For our purposes here, forces are either (1) contact forces, applied by a push or a pull through direct contact, or they are field forces, such as gravity. The first group, the contact forces, require that something be "attached" to the object to apply the force, such as a rope, a floor, or a hand, all of which are "in contact" with the object. Gravity, on the other hand, acts at a distance, without any direct agent to apply it. Thus a satellite in Earth orbit is subject to Earth's gravity, even though there is no agent (a rope, a hand, etc) to apply it.
 
Alright, so i got these two equations now, am I on the right track or did I go wrong somewhere?

ΣFx = m*a = mgSinθ - T
Σtorque = I*α = ½Mr^2*α= ½Mr^2*(a/r)edit: Nvm I got the correct answer

I used ΣFx = m*a = mgSinθ - T to find my tension and worked on from there

Thanks a lot for your help!
 
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Kindly see the attached pdf. My attempt to solve it, is in it. I'm wondering if my solution is right. My idea is this: At any point of time, the ball may be assumed to be at an incline which is at an angle of θ(kindly see both the pics in the pdf file). The value of θ will continuously change and so will the value of friction. I'm not able to figure out, why my solution is wrong, if it is wrong .
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