![]() In general, the moment of inertia is a tensor, see below. This article mainly considers symmetric mass distributions, with constant density throughout the object, and the axis of rotation is taken to be through the center of mass unless otherwise specified.įollowing are scalar moments of inertia. When calculating moments of inertia, it is useful to remember that it is an additive function and exploit the parallel axis and perpendicular axis theorems. In general, it may not be straightforward to symbolically express the moment of inertia of shapes with more complicated mass distributions and lacking symmetry. ![]() Typically this occurs when the mass density is constant, but in some cases the density can vary throughout the object as well. It should not be confused with the second moment of area, which is used in bending calculations.įor simple objects with geometric symmetry, one can often determine the moment of inertia in an exact closed-form expression. ![]() ![]() Mass moments of inertia have units of dimension × 2. In physics and applied mathematics, the mass moment of inertia, usually denoted by Template:Mvar, measures the extent to which an object resists rotational acceleration about an axis, and is the rotational analogue to mass.
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