The mass moment of inertia Θa is determined from
We can determine the geometrical relations
r = R + c sinϕ ,
dm = ρ 2πr2c cosϕ dr
from the figure. With
dr = c cosϕ dϕ
we obtain
Note that the integrals of the odd functions over the even interval are zero. Using m = 2π2ρc2R we finally get
This result reduces to Θa = mR2 in the case of a thin ring (c ≪ R).