What is the derivation of the moment of inertia of a solid sphere?

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SUMMARY

The moment of inertia of a solid sphere is derived by summing the contributions of infinitesimally small disks, each with mass dm. The term (1/2)y² arises from the formula for the moment of inertia of a disk, which is (1/2)MR², where R is the radius of the disk. The derivation process involves integrating these contributions across the entire volume of the sphere. Different approaches to defining mass elements, such as dm = dfg dr versus dI = abc dm, can lead to confusion, but both methods ultimately aim to achieve the same result.

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piquante
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So here I just need help understanding a concept.
I was reading this website's derivation of the moment of inertia of a solid sphere here: http://hyperphysics.phy-astr.gsu.edu/hbase/isph.html#sph3
For the life of me I can't see where the (1/2)y2 term comes from. I would understand y2 because that would be the radius, but the 1/2?
I understand the other steps but I'm very much stuck on this first one.

A related question for anyone who has an opinion: this website starts out these problems by writing dI = abc dm. My physics professor tends to start with dm = dfg dr. Is there a best way to approach these problems? I'm always the most confused at the beginning when I need to define the above relationships. Thanks!
 
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To find the moment of inertia of the sphere, they had to sum the moment of inertia of many tiny disks of mass dm. The moment of inertia of a disk of mass M is (1/2)MR^2. To see a derivation of the moment of inertia of a disk: http://mikebloxham.com/H7A/I for sphere.pdf
 

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