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Line 42: \| pages = 791–795 \| title = Generalization of parallel axis theorem for rotational inertia \| volume = 85\| doi-access = free ~~\| volume = 85~~}}</ref> Let {{math\|''I<sub>ij</sub>''}} denote the inertia tensor of a body as calculated at the center of mass. Then the inertia tensor {{math\|''J<sub>ij</sub>''}} as calculated relative to a new point is :<math>J_{ij}=I_{ij} + m\left(\|\mathbf{R}\|^2 \delta_{ij}-R_i R_j\right),</math>

Parallel axis theorem: Difference between revisions