EN to the parallel axis theorem.

NAhild's method is correct except for equating a to g. The correct acceleration is a=2g/3. Therefore the correct tension is T=Mg(1-2/3)=Mg/3. In summary, the conversation discusses how to find the tension in a string attached to a fixed rod and a uniform disk. The correct method involves setting the net torque equal to the moment of inertia multiplied by the angular acceleration, and using the parallel axis theorem to find the moment of inertia about the point of rotation. The resulting tension is shown to be equal to one-third of the weight of the disk.
  • #1
thenewbosco
187
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I have a diagram for this at http://snipurl.com/diagr

There is a uniform disk with radius R, mass M, it has a string wrapped around it and is attached to a fixed rod.
Part 1: Show the tension in the string is 1/3 the weight of the disk

what i have done for this is

[tex] Torque=Fd [/tex]
and setting the force equal to Tension
[tex] Torque=TR [/tex]
then [tex] \sum Torque=I\frac{a}{R}[/tex] and i used [tex]I=\frac{1}{2}MR^2[/tex]for the moment of inertia

Then [tex] TR=\frac{1}{2}MRa[/tex]
[tex]T=\frac{1}{2}Ma[/tex]
and then acceleration is just g, so i get the tension equals 1/2 the weight. where have i gone wrong?
 
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  • #2
thenewbosco said:
I have a diagram for this at http://snipurl.com/diagr

There is a uniform disk with radius R, mass M, it has a string wrapped around it and is attached to a fixed rod.
Part 1: Show the tension in the string is 1/3 the weight of the disk

what i have done for this is

...
[tex]T=\frac{1}{2}Ma[/tex]
and then acceleration is just g, so i get the tension equals 1/2 the weight. where have i gone wrong?

The acceleration of the centre of mass is not just g, but it is determined by the resultant of all forces acting on the pulley.

ehild
 
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  • #3
thenewbosco said:
where have i gone wrong?
Your method is correct except for equating a to g. The forces are Mg and T, so Mg-T=ma. You have found that T = Ma/2 so T = Mg/3. Here is another way of looking at it:

The weight is Mg. The tension is T. The net force provides the acceleration of the wheel:

(1) Mg - T = Ma

To find the acceleration of the center of mass:
The torque of the center of mass about the point of rotation (point of contact between wheel and string) is MgR. That torque divided by the moment of inertia of the wheel about that contact point provides the angular accleration of the centre of mass = a/R.

So:

(2)[tex]MgR/I = a/R [/tex]

The moment of inertia about that point is NOT the same as the moment of inertia about the center. Use the parallel axis theorem: [itex]I = I_{centre} + MR^2 = \frac{1}{2}MR^2 + MR^2 = \frac{3}{2}MR^2[/itex]

Plugging that into (2) results in a = 2g/3

Then it is just a matter of plugging that into (1) to get:

T = Mg(1 - 2/3) = Mg/3

AM
 
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FAQ: EN to the parallel axis theorem.

What is the "Uniform disk tension problem"?

The uniform disk tension problem is a physics problem that involves calculating the tension in a string or rope that is attached to a uniform disk and being pulled at a certain angle.

What are the key factors that affect the tension in the string?

The key factors that affect the tension in the string are the mass of the disk, the angle at which the string is being pulled, and the coefficient of friction between the string and the disk.

How is the tension calculated in this problem?

The tension in the string can be calculated by using the equation T = mg/(cosθ + μsinθ), where T is the tension, m is the mass of the disk, g is the acceleration due to gravity, θ is the angle at which the string is being pulled, and μ is the coefficient of friction.

What is the purpose of solving this problem?

The purpose of solving this problem is to understand the relationship between tension, mass, angle, and coefficient of friction in a real-world scenario. This problem can also help in understanding the concept of equilibrium and how forces are distributed in a system.

Are there any real-world applications of the uniform disk tension problem?

Yes, the uniform disk tension problem has many real-world applications, such as in engineering and construction, where understanding the tension in ropes and cables is crucial for ensuring the stability and safety of structures. It is also relevant in sports, such as rock climbing and sailing, where tension in ropes and cables is used to support and maneuver objects.

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