the moment of inertia of a solid hemisphere of mass M and radius R about an axis passing through its centre of mass and parallel to its circular face is
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Since the center of mass of a solid hemisphere is 3/8 R above the circular base; so reducing it to a one particle system, and the moment of inertia of that one particle system isM(
8R
3
)
2
=M
64
9
×R
2
Now moment of inertia of the particle about an axis parallel to the original one but at a distance of 3/4 R can be obtained using the parallel axis theorem
new M.I = MR
2
64
45
so the radius of gyration =R(
64
45
)
2
1
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