Introductory Physical Pendulum Problem

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SUMMARY

The discussion focuses on solving a physical pendulum problem involving a thin rod and a uniform sphere. The period of oscillation is calculated using the formula T = 2π√(I/mgd), where I is the moment of inertia. Participants emphasize the importance of correctly applying the parallel axis theorem to find the moment of inertia for the sphere and the rod. The correct approach involves calculating the inertia of both components about the pivot point and combining them to determine the overall moment of inertia.

PREREQUISITES
  • Understanding of physical pendulum dynamics
  • Knowledge of moment of inertia calculations
  • Familiarity with the parallel axis theorem
  • Basic grasp of angular motion equations
NEXT STEPS
  • Study the application of the parallel axis theorem in detail
  • Learn how to derive the moment of inertia for composite bodies
  • Explore the derivation of the period of a physical pendulum
  • Practice solving similar problems involving pendulums and rotational dynamics
USEFUL FOR

Physics students, educators, and anyone interested in understanding the dynamics of physical pendulums and rotational motion.

Zipzap
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Homework Statement


A pendulum is constructed using a thin rod (m1 = 2.0 kg, L = 1.0m) and a uniform sphere (m2 = 1.0 kg, R = 0.50 m). The period in "s" for small oscillations is:
a) 1.5
b) 1.7
c) 2.0
d) 2.2
e) 2.5


Homework Equations


T = 2pi *sqrt(I/mgd)


The Attempt at a Solution


To start off, the rod is pivoting at an end attached to a ceiling with the sphere attached to its bottom.
I initially got (c) by assuming it was a simple pendulum ("thin rod", lol), but a more careful look reveals that the rod does not have negligible mass, and so this pendulum must be physical. My biggest dilemma with this problem is finding the center of mass for this system, and then finding "d" assuming that. Unfortunately, inertia is my weakest area in Physics, and so I am stuck as to how to use the parallel axis theorem correctly to get my answer.
Any hints?
If it helps, people in my class keep getting (d) or (e).
 
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show an attempt on finding moment of inertia and center of mass.
 
All right, here goes nothing =P

I know that the rod has inertia of (1/3)ML^2, and the sphere has (2/5)MR^2...

I also know I = integral of r^2, r = L+R...

Am I on the right track here?
 
take inertia about the point of suspension.
 
What do you mean by that? You mean where the rod is being suspended?
 
Zipzap said:
All right, here goes nothing =P

I know that the rod has inertia of (1/3)ML^2, and the sphere has (2/5)MR^2...
About which axis.
You have to take moment of inertia about line perpendicular to the plane in which pendulum swings and passing through point of suspension
 
So then I can just simply add inertias for both the rod and sphere to get my moment of inertia?
 
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yes right. proceed that way.
 
  • #10
And I can add them both because the pivot point is unchanged and the sphere itself contributes to the overall inertia, right?

Anyhow, I get (1/3)ML^2 + (2/5)MR^2, giving me a numerical value of 0.7666666 when I sub in my values.

What do I do about "d" when I input it into the formula for periods? =S
 
  • #11
Zipzap said:
Anyhow, I get (1/3)ML^2 + (2/5)MR^2, giving me a numerical value of 0.7666666 when I sub in my values.

No. The moment of inertia of the sphere is not (2/5)MR^2 about the required axis. It is (2/5)MR^2 about its. You will need to find its moment of inertia about the required axis using parallel axis theorem.
 
  • #12
About its axis? But it's attached to the rod, how am I supposed to find it using parallel axis theorem??
 
  • #13
the distance of the centre of sphere from point of suspension is equal to length of rod.
 
  • #14
Ok, now I'm confused:

I know that I have to add the inertias together. The sphere will have a different inertia that I have find using the parallel axis theorem (no clue how to do this), and without the center of gravity, I have no idea how to find "d"

Any other helpful advice?
 
  • #15
ok, let us start from the basics. When you want to find angular acceleration, you find it about an axis of rotation. Now, how do you find it? You calculate torque about that axis and the moment of inertia about that axis. Now, you have a relation:
\tau = I \alpha

In your question the axis to be taken is the one mentioned earlier. For using the above relation you have to calculate moment of inertia about about that axis. Now, you know that moment of inertia of the sphere is 2/5 Mr^2 about its diameter. also distance between diameter and that axis is the length of the string.

using parallel axis theorem moment of inertia of the sphere is 2/5 Mr^2 + ML^2 where L is the length of the string.
 

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