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m in parallel axis theorem of mass moment of inertia, the parallel axis is parallel to the axis passes through the centre of mass of the body instead of its centre of gravity. |
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=== Tensor generalization ===
The parallel axis theorem can be generalized to calculations involving the [[Moment of inertia#
:<math>J_{ij}=I_{ij} + m\left(|\mathbf{R}|^2 \delta_{ij}-R_i R_j\right),</math>
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