Period of Oscillation for a Hoop of Mass 0.420 kg & Radius 0.130 m

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Homework Help Overview

The discussion revolves around the period of oscillation for a hoop suspended at a point on its perimeter, exploring the dynamics of small oscillations and the relevant formulas for calculating the period. Participants also touch on a related problem involving a mass on a spring and energy decay due to friction.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants attempt to derive the period of oscillation using different expressions for rotational inertia and question the assumptions regarding the center of mass and the axis of rotation.
  • Some participants explore the relationship between amplitude and total energy in oscillatory motion, raising questions about the energy decay process.
  • There is a discussion about the correctness of the formulas used and the interpretation of the physical setup, particularly regarding the rotational inertia of the hoop.

Discussion Status

The discussion is ongoing, with participants providing feedback on each other's approaches and questioning the validity of certain assumptions. Some guidance has been offered regarding the formulas for rotational inertia, but no consensus has been reached on the correct approach or solution.

Contextual Notes

Participants are working under the constraints of homework rules, which may limit the information available for resolving the problems. There are also indications of confusion regarding the setup of the problems and the application of physical principles.

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A hoop of radius 0.130 m and mass 0.420 kg is suspended by a point on its perimeter as shown in the figure. If the hoop is allowed to oscillate side to side as a pendulum, what is the period of small oscillations?

T = 2pi (mgl/I)^.5

I assume that l = r, since center of mass is in the middle of the hoop.
I = 3mr^2/2

So T = 2pi(2g/3r)

Also tried with I = mr^2/2 in case I'm misunderstanding the problem and it is oscillating in the other direction, but this did not work either.

Anyone see my error?

Next:
A mass M is suspended from a spring and oscillates with a period of 0.860 s. Each complete oscillation results in an amplitude reduction of a factor of 0.965 due to a small velocity dependent frictional effect. Calculate the time it takes for the total energy of the oscillator to decrease to 0.500 of its initial value.

Tried .965^t = .5, then t = log(.5)/log(.965) but this didn't work... any other suggestions?
 
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squib said:
A hoop of radius 0.130 m and mass 0.420 kg is suspended by a point on its perimeter as shown in the figure. If the hoop is allowed to oscillate side to side as a pendulum, what is the period of small oscillations?

T = 2pi (mgl/I)^.5

I assume that l = r, since center of mass is in the middle of the hoop.
I = 3mr^2/2

So T = 2pi(2g/3r)

Also tried with I = mr^2/2 in case I'm misunderstanding the problem and it is oscillating in the other direction, but this did not work either.

Anyone see my error?
Two problems:
Check your formula for the period of a pendulum (you have terms upside down).
Check your value for the rotational inertia.
 
squib said:
A mass M is suspended from a spring and oscillates with a period of 0.860 s. Each complete oscillation results in an amplitude reduction of a factor of 0.965 due to a small velocity dependent frictional effect. Calculate the time it takes for the total energy of the oscillator to decrease to 0.500 of its initial value.

Tried .965^t = .5, then t = log(.5)/log(.965) but this didn't work... any other suggestions?
How does amplitude relate to total energy? (It's the energy that decreases by half, not the amplitude.)
 
I can't seem to find the right I... isn't 3mr^2/2 right for a ring rotated about a line tangent to the circle?
 
I tried I = (MR^2)/2 + MR^2 = (3/2)MR^2

T = 2pi * Sqrt(3/2 MR^2/MgR) = 2pi * Sqrt((3/2)r/g))

This didn't work is there something I missed?
 
squib said:
I can't seem to find the right I... isn't 3mr^2/2 right for a ring rotated about a line tangent to the circle?
Ah... here's where a picture would help. If the ring rotates through an axis tangent to the circle, then that would be correct. On the other hand, if the ring rotated on an axis perpendicular to its plane, the rotational inertia would be: I = 2mr^2. (That's how I interpreted the problem, but you are the one with the diagram!)
 

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