Inertia of a solid vertical disk about it's diameter

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SUMMARY

The moment of inertia of a solid, uniform density disk rotating about its diameter is derived using calculus, specifically through the integration of infinitesimal inertia contributions from vertical rods. The relevant equations include the inertia of a thin vertical rod, expressed as I = m*x^2, and the area density σ = M/A, where A = π*R². The integration process involves substituting y in terms of x using the Pythagorean theorem, leading to the final result of I = 1/4 MR². The discussion emphasizes the necessity of calculus knowledge, particularly in handling integration without double integrals.

PREREQUISITES
  • Understanding of calculus, specifically integration techniques
  • Familiarity with the concept of moment of inertia
  • Knowledge of area density and its calculation
  • Basic geometry, particularly the Pythagorean theorem
NEXT STEPS
  • Study integration techniques for calculating moment of inertia in different shapes
  • Learn about the derivation of moment of inertia for various geometric bodies
  • Explore the application of area density in physics problems
  • Investigate the use of trigonometric substitutions in integrals
USEFUL FOR

Physics students, mechanical engineers, and anyone interested in understanding the principles of rotational dynamics and moment of inertia calculations.

DaveyThompson
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Homework Statement



Derive the moment of inertia of a solid, uniform density, disk rotating about a diameter using vertical rods.
Diagram: http://i.imgur.com/TQIjz.png

Only the radius of the circle and the inertia of a thin rod is given

Homework Equations


Inertia of thin vertical rod = m*r^2
σ= area density
M= Total mass
I= inertia
dm= infinitesimal amount of mass
dI= infinitesimal amount of inertia
A= total area
R= radius of the circle

The Attempt at a Solution


This is the method given in my class. Because calculus 1 is the only prerequisite we can not use double integrals.I of rod = m*x^2
dI= dm
*x^2
dm=σ*da
da= 2y*dx
σ= M/A
A=pi*R^2
σ= M/(pi*R^2)
dm=M/(pi*R^2) * 2y*dx
dI= M/(pi*R^2) * 2y*x^2 * dxFrom here we have to put y in terms of x which I think must be done using the Pythagorean theorem so:
y=(R^2-x^2)^(1/2)

subbing in we get:

dI= M/(pi*R^2) * 2(R^2-x^2)^(1/2) * x^2 * dx

This is why I get stuck because I am not quite sure how to integrate that. What is should come out to be is I = 1/4 MR^2. If anyone can offer an explanation it would be very appreciated.
 
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try substituting x=Rsin(theta).
 

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