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Radius of Gyration

For a planar distribution of mass rotating about some axis in the plane of the mass, the radius of gyration is the distance from the axis that all mass can be concentrated to obtain the same mass moment of inertia. Thus, the radius of gyration is the ``equivalent distance'' of the mass from the axis of rotation. In this context, gyration can be defined as rotation of a planar region about some axis lying in the plane.

For a bar cross-section with area $ S$, the radius of gyration is given by

$\displaystyle r_{\underline{x}} = \sqrt{\frac{I_{S,\underline{x}}}{S}} \protect$ (F.7)

where $ I_{S,\underline{x}}$ is the area moment of inertiaF.4.4) of the cross-section about the line $ \underline{x}$ lying in the plane of the cross-section (usually passing through its centroid):

$\displaystyle I_{S,\underline{x}} = \int_S r_{\underline{x}}^2 dS,
$

where $ r_{\underline{x}}$ denotes the distance of the differential area element $ dS$ from the axis of gyration (line $ \underline{x}$).



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written by Julius Orion Smith III
Julius Smith's background is in electrical engineering (BS Rice 1975, PhD Stanford 1983). He is presently Professor of Music and Associate Professor (by courtesy) of Electrical Engineering at Stanford's Center for Computer Research in Music and Acoustics (CCRMA), teaching courses and pursuing research related to signal processing applied to music and audio systems. See http://ccrma.stanford.edu/~jos/ for details.