Roman C. answered 08/27/15
Tutor
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Masters of Education Graduate with Mathematics Expertise
You don't need the perpendicular distance to L.
Tables of moments of inertia usually mention the circular disk plate about the axis of rotation, which is mr2/2
Placing it on the x-y plane, this is Iz and by the perpendicular axis theorem for flat plates, Ix+Iy = Iz so Ix = Iy = mr2/4
For an ellipse with axis of length 2a on the x-axis and 2b on the y-axis, we have
Ix = mb2/4, Iy = ma2/4 and Iz = m(a2+b2)/4
The products of inertia Ixy = ∫xy dm, etc. are all 0 by symmetry.
So the inertia tensor is I =
[Ix 0 0]
[0 Iy 0]
[0 0 Iz]
[0 Iy 0]
[0 0 Iz]
We need the inertia tensor I' in the rotated system by k counterclockwise about the z-axis where the x-axis will be along line L. The matrix of the rotation transformation is S =
[cos k -sin k 0]
[sin k cos k 0]
[ 0 0 1]
[sin k cos k 0]
[ 0 0 1]
And S-1 is a clockwise rotation.
[ cos k sin k 0]
[-sin k cos k 0]
[ 0 0 1]
[-sin k cos k 0]
[ 0 0 1]
The transformed inertia tensor is the matrix product I' = S-1IS =
[ Ix cos2 k + Iy sin2 k (Ix-Iy)sin k cos k 0]
[ (Ix-Iy)sin k cos k Ix sin2 k + Iy cos2 k 0]
[ 0 0 Iz]
[ (Ix-Iy)sin k cos k Ix sin2 k + Iy cos2 k 0]
[ 0 0 Iz]
So The moment of inertia about L is
IL = Ix' = Ix cos2 k + Iy sin2 k = m(b2cos2k + a2sin2k)/4.