The moment of inertia with respect to a given axis of a solid body with density is defined by the volume integral
(1)
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where is the perpendicular distance from the axis of rotation. This can be broken into components as
(2)
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for a discrete distribution of mass, where is the distance to a point (not the perpendicular distance) and is the Kronecker delta, or
(3)
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for a continuous mass distribution. Depending on the context, may be viewed either as a tensor or a matrix. Expanding (3) in terms of Cartesian axes gives the equation
(4)
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The moment of inertia of a region can be computed in the Wolfram Language using MomentOfInertia[reg].
The moment of inertia tensor is symmetric, and is related to the angular momentum vector by
(5)
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where is the angular velocity vector.
The principal moments of inertia are given by the entries in the diagonalized moment of inertia matrix, and are denoted (for a solid) , , and in order of decreasing magnitude. In the principal axes frame, the moments are also sometimes denoted , , and . The principal axes of a rotating body are defined by finding values of such that
(6)
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(7)
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which is an eigenvalue problem.
The following table summarizes the moments of inertia of some common solids around some of their principal axes.
solid/axis | moment of inertia |
cylinder about symmetry axis | |
cylinder about central diameter | |
ellipsoid about principal axis | |
elliptical slab about major axis | |
elliptical slab about vertical | |
cuboid about major axis | |
ring about perpendicular axis | |
ring about diameter | |
rod about end | |
rod about center | |
sphere about diameter | |
spherical shell | |
torus about diameter | |
torus about symmetry axis |