Center of Mass and Mass Moments of Inertia for Homogeneous 3D Bodies
- Page ID
- 58319
Shape with Volume and Center of Mass Location Shown | Mass Moments of Inertia |
---|---|
Slender Rod |
\(I_{xx} = I_{zz} = \dfrac{1}{12} ml^2\) \(I_{yy} = 0\) \(I_{xx'} = I_{zz'} = \dfrac{1}{3} ml^2\) |
Flat Rectangular Plate |
\(I_{xx} = \dfrac{1}{12} mh^2\) \(I_{yy} = \dfrac{1}{12} m (h^2 + b^2) \) \(I_{zz} = \dfrac{1}{12} mb^2\) |
Flat Circular Plate |
\(I_{xx} = I_{zz} = \dfrac{1}{4} mr^2\) \(I_{yy} = \dfrac{1}{2} mr^2\) |
Thin Circular Ring |
\(I_{xx} = I_{zz} = \dfrac{1}{2} mr^2\) \(I_{yy} = mr^2\) |
Rectangular Prism \(Volume = dwh\) |
\begin{align*} I_{xx} &= \frac{1}{12} m(h^2 + d^2) \\[4pt] I_{yy} &= \frac{1}{12} m(d^2 + w^2) \\[4pt] I_{zz} &= \frac{1}{12} m(h^2 + w^2) \end{align*} |
Cylinder \(Volume = \pi r^2 h\) |
\( I_{xx} = I_{zz} = \dfrac{1}{12} m(3r^2 + h^2) \) \(I_{yy} = \dfrac{1}{2} mr^2\) |
Thin Cylindrical Shell |
\(I_{xx} = I_{zz} = \dfrac{1}{6} m(3r^2 + h^2)\) \(I_{yy} = mr^2\) |
Half Cylinder \(Volume = \dfrac{1}{2} \pi r^2h\) |
\(I_{xx} = I_{zz} = \left( \dfrac{1}{4} - \dfrac{16}{9 \pi^2} \right) mr^2 + \dfrac{1}{12} mh^2\) \(I_{yy} = \left( \dfrac{1}{2} - \dfrac{16}{9 \pi^2} \right) mr^2\) \(I_{xx'} = I_{zz'} = \dfrac{1}{12} m(3r^2 + h^2)\) \(I_{yy'} = \dfrac{1}{2} mr^2\) |
Sphere \(Volume = \dfrac{4}{3} \pi r^3\) |
\(I_{xx} = I_{yy} = I_{zz} = \dfrac{2}{5} mr^2\) |
Spherical Shell |
\(I_{xx} = I_{yy} = I_{zz} = \dfrac{2}{3} m r^2\) |
Hemisphere \(Volume = \dfrac{2}{3} \pi r^3\) |
\(I_{xx} = I_{zz} = \dfrac{83}{320} mr^2\) \(I_{yy} = \dfrac{2}{5} mr^2\) \(I_{xx'} = I_{zz'} = \dfrac{2}{5} mr^2\) |
Hemispherical Shell |
\(I_{xx} = I_{zz} = \dfrac{5}{12} mr^2\) \(I_{yy} = \dfrac{2}{3} mr^2\) \(I_{xx'} = I_{zz'} = \dfrac{2}{3} mr^2\) |
Right Circular Cone \(Volume = \dfrac{1}{3} \pi r^2 h\) |
\(I_{xx} = I_{zz} = \dfrac{3}{80} m(4r^2 + h^2) \) \(I_{yy} = \dfrac{3}{10} mr^2\) \(I_{xx'} = I_{zz'} = \dfrac{1}{20} m(3r^2 + 2h^2) \) |