The perpendicular axis theorem, also called the plane figure theorem, is a result used to compute the moment of inertia of a flat, two dimensional object known as a planar lamina. It states that the moment of inertia of such an object about an axis perpendicular to its plane equals the sum of the moments of inertia about two axes that lie within the plane itself, are perpendicular to each other, and intersect at the point where the perpendicular axis passes through the object. The theorem applies only to objects that lie entirely within a single plane. It is often used together with the parallel axis theorem to calculate the polar moment of inertia for a variety of shapes, and when a planar object has enough rotational symmetry that its two in plane moments of inertia are equal, the theorem simplifies further into a particularly useful relationship between the perpendicular moment and either of the equal in plane moments.
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StatementFor a planar lamina, the moment of inertia about an axis perpendicular to its plane equals the sum of the moments of inertia about two mutually perpendicular axes in the plane meeting at the point where the perpendicular axis passes through (Iz = Ix + Iy). 1 Classification
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Source Perpendicular axis theorem (Wikipedia)
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1. Perpendicular axis theorem (Wikipedia)
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for a planar lamina the moment of inertia about an axis perpendicular to the plane of the lamina is equal to the sum of the moments of inertia about two mutually perpendicular axes in the plane of the lamina, which intersect at the point where the perpendicular axis passes through.
In Group: Classical Mechanics and Dynamics, Lead section
plane figure theorem) states that for a planar lamina the moment of inertia about an axis perpendicular to the plane of the
In Branch: Mathematical Physics, Lead section
plane figure theorem) states that for a planar lamina the moment of inertia about an axis perpendicular to the plane of the
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