How Long Does It Take for a Disc to Stop Under Applied Force?

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Homework Help Overview

The discussion revolves around a physics problem involving a vertical disc subjected to an applied force, with the aim of determining the time it takes for the disc to come to a momentary stop. The problem includes parameters such as mass, radius, initial angular velocity, and the distance of the applied force from the center of the disc.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the moment of inertia calculation and the application of torque in relation to angular acceleration. Questions arise regarding the definitions of variables and the correct application of equations, including the relationship between force, torque, and angular motion.

Discussion Status

The discussion is active, with participants providing feedback on each other's reasoning and calculations. Some guidance has been offered regarding the use of torque and angular acceleration equations, while others are exploring different interpretations of the problem setup.

Contextual Notes

Participants are working within the constraints of a textbook problem that does not provide a solution, prompting them to verify their understanding and approach to the physics concepts involved.

sauri
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Help please!

I found this question in my textbook but the solution is not stated. A force of 2 N vertically down is applied to a vertical disc at a distance 2 cm to the right (horizontally) of the centre of the disc. The disc has a mass of 1.2 kg and a radius of 15 cm. Its initial angular velocity is 2 rad.s-1 anticlockwise.

How long does it take to come to a (momentary) stop?

I took a crack at it but is it correct?.
I=(mr^2)/2, I=[1.2x(15/100)^2]2. Then the value for I is substituted to F=Ia, where 2=value for Ixa, where a is found, and then substitute for a=w/t. So a is substituted=2/t and t is found.

Is this o.k?
 
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sauri said:
I took a crack at it but is it correct?.
I=(mr^2)/2, I=[1.2x(15/100)^2]2. Then the value for I is substituted to F=Ia, where 2=value for Ixa, where a is found, and then substitute for a=w/t. So a is substituted=2/t and t is found.

Is this o.k?
The equation must be [itex]M=Fd=I\ddot{\theta}[/itex][/color]
 
The M represents what exactly? and isn't the momentum for a disk about it's center I = ½ mr2?
 
I believe the M is turning moment or torque. Your F = Ia equation needs modifing, instead of using F, you must use torque:
[tex]\tau = I\alpha[/tex]
This is a version of Newton's second law.
 
I see, but is the working correct?
 
sauri said:
I found this question in my textbook but the solution is not stated. A force of 2 N vertically down is applied to a vertical disc at a distance 2 cm to the right (horizontally) of the centre of the disc. The disc has a mass of 1.2 kg and a radius of 15 cm. Its initial angular velocity is 2 rad.s-1 anticlockwise.

How long does it take to come to a (momentary) stop?

I took a crack at it but is it correct?.
I=(mr^2)/2, I=[1.2x(15/100)^2]2. Then the value for I is substituted to F=Ia, where 2=value for Ixa, where a is found, and then substitute for a=w/t. So a is substituted=2/t and t is found.

Is this o.k?

The first part is allright. After finding a(angular acceleration) you need to
use the eqn

[tex]\omega_{f}=\omega_{i}+at[/tex]

Now solve for t putting [tex]\omega_{f}=0[/tex]

I recommend you go through the eqns of motion for angular variables.

Edit:I didn't read ur sol properly.You also need to use [tex]\tau=Ia[/tex]
and substitute [tex]\tau=rF[/tex]
 
Last edited:
You are quite right arundg, it would be a lot simpler using equations of motion, I didn't stop to consider the question, I was simply looking for errors.
 
I thank you all for your help. But could you tell me what the T in the equation T=rF stands for. Thanks again!
 
[itex]\tau = rF[/itex] is simply torque, force([itex]F[/itex]) multiplied by distance([itex]r[/itex]) from the axis of rotation.
 
Last edited:
  • #10
Edit:I didn't read ur sol properly.You also need to use [tex]\tau=Ia[/tex]
and substitute [tex]\tau=rF[/tex][/QUOTE]

I understand using the [tex]\tau=Ia[/tex] part where we can find [tex]\alpha[/tex](angular acceleration). But why do we need to substitue [tex]\tau=rF[/tex]?. Why can we not just find [tex]\alpha[/tex], and find t so it can be substituted into [tex]\omega_{f}=\omega_{i}+at[/tex]
 
Last edited:
  • #11
You need to use [itex]\tau = rF[/itex] and put it equal to [itex]\tau = I\alpha[/itex] to find the angular accelertatiion thus;

[tex]I\alpha = rF[/tex]

[tex]\alpha = \frac{rF}{I}[/tex]

Can you go from here?
 
  • #12
got it.thanks
 
  • #13
No problem
 

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