Rotational Motion of Masses Problem

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SUMMARY

The discussion focuses on calculating the moment of inertia for slotted masses in a physics lab on rotational motion. Participants emphasize the need to model the masses as disks of uniform density rather than point masses, utilizing the parallel-axis theorem for accurate calculations. Key equations include τ = r x F, τ = I α, and I = I (cm) + Mh². The conversation highlights the importance of deriving the moment of inertia considering the cut-out slots and comparing theoretical values with experimental data.

PREREQUISITES
  • Understanding of rotational motion concepts, specifically moment of inertia.
  • Familiarity with the parallel-axis theorem in physics.
  • Knowledge of torque equations and their applications.
  • Ability to derive equations for complex shapes, such as disks with cut-out slots.
NEXT STEPS
  • Study the parallel-axis theorem in detail to apply it effectively in calculations.
  • Learn how to derive the moment of inertia for composite shapes, including disks with cut-outs.
  • Explore experimental methods for measuring moment of inertia in lab settings.
  • Review torque equations and their implications in rotational dynamics.
USEFUL FOR

Students in physics courses, particularly those working on rotational motion experiments, and educators seeking to clarify concepts related to moment of inertia and its calculations.

wizzpowa
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Homework Statement



Hey all - I'm doing a physics lab on rotational motion, and I can not make sense of the last part, the additional analysis. The question is:

Since our masses are not actually point-masses, the theoretical model I = MR^2 is not very accurate, so for a better theoretical comparison we
should assume that each of the slotted masses is a disk of uniform density (neglect the effect of the slot) instead of a point mass. The moment of inertia for a single disk about an axis through the center of mass and parallel to the face of the disk is shown in the figure at right, where M is the mass of the disk, R is the radius of the disk and L is the thickness of the disk. You will need to use the parallel-axis theorem, check your textbook for details. Is this theoretical value in better agreement with the experimental data? Can you derive an equation to determine the moment of inertia of the masses including the cut-out slots? How does this value compare to the measured moment of inertia?

This is due in the next hour and a half, and I've been trying to make sense of it for over an hour. How can we equate the parallel-axis theorem to what they give us in the problem?

Homework Equations



τ = r x F
τ = I α
I = I (cm) + Mh^2
I = I(0) + Ii
I (cm) = (1/4)Mr^2 + (1/3)ML^2

The Attempt at a Solution



Because it is more of a conceptual problem, I am not sure where to even start. If someone could help me out, it would mean a lot! Thanks! If you need more information about the lab, let me know.
 
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hi wizzpowa! :smile:

hmm … half an hour to go …

i'm not sure what your question is :confused:

if the mass is a disc of mass m and diameter r at distance R from the centre of rotation, O,

then the moment of inertia IO about O is mR2 plus IC, the moment of inertia about the centre of the disc, C,

and τC = ICα :wink:
 
hi wizzpowa! :smile:

thanks for the pm

as always on this forum, you need to show us your work!

(or at least the bit that's bothering you)
 

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