Derivation of moment inertia formula

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SUMMARY

The derivation of the moment of inertia formula for a uniform thin rod about an axis through its center is established as 1/12 Ml². This is achieved by integrating the expression for moment of inertia, I = ∫ R² dm, where dm is expressed in terms of density (p), cross-sectional area (A), and differential length (dx). The integration limits are set from -l/2 to l/2, leading to the result of 1/12 pAl³, which simplifies to 1/12 Ml² when substituting mass (M) as pAl.

PREREQUISITES
  • Understanding of integral calculus
  • Familiarity with the concept of moment of inertia
  • Knowledge of mass density and its relation to volume
  • Basic principles of mechanics and rigid body dynamics
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  • Study the derivation of moment of inertia for different shapes, such as cylinders and spheres
  • Learn about the parallel axis theorem and its applications
  • Explore the relationship between moment of inertia and angular momentum
  • Investigate the role of moment of inertia in rotational dynamics
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How do I derive the formula 1/12 Ml^2?
Derive the formula for moment of inertia of a uniform thin rod of length l about an axis through its center perpendicular to the rod.
 
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There are a few ways to do it. Moment of inertia is calculated by
\int R^2.dm

So place x=0 at the centre, the x-axis running along the rod. So you're integrating from -l/2 to l/2.
We must find dm in terms of our integration variable x. In dx we have an element of mass dm.
mass = (density)(volume)=(density)(cross-sectional area)(length)

So
dm = p.A.dx
where p is the density and A the cross-sectional area. Our integral is now:
\int_{-l/2}^{l/2} pAx^2.dx
If you work it out you find it equals:
\frac{1}{12} pAl^3

but if we remember that mass = pAl, then we get 1/12 Ml^2.
 

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