EN to the parallel axis theorem.

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SUMMARY

The discussion centers on the application of the parallel axis theorem to determine the tension in a string wrapped around a uniform disk with radius R and mass M. The correct derivation shows that the tension T in the string is one-third the weight of the disk (T = Mg/3). The error in the initial calculation was equating the acceleration of the center of mass directly to g, rather than accounting for the net forces acting on the system. The moment of inertia used in the calculations must reflect the parallel axis theorem, resulting in I = (3/2)MR².

PREREQUISITES
  • Understanding of torque and its relation to force (Torque = Fd)
  • Familiarity with moment of inertia and its calculations (I = 1/2 MR²)
  • Knowledge of the parallel axis theorem and its application
  • Basic principles of dynamics, including Newton's second law (F = ma)
NEXT STEPS
  • Study the parallel axis theorem in detail and its implications for rotational dynamics
  • Learn about the derivation of moment of inertia for various shapes and axes
  • Explore the relationship between linear and angular acceleration in rotational systems
  • Investigate real-world applications of torque and tension in mechanical systems
USEFUL FOR

Students of physics, mechanical engineers, and anyone interested in understanding rotational dynamics and the application of the parallel axis theorem in problem-solving.

thenewbosco
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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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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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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 acceleration 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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