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Inertia tensor of triangle : ウィキペディア英語版
Inertia tensor of triangle

The inertia tensor
\mathbf of a triangle (like the inertia tensor of any body) can be expressed in terms of covariance
\mathbf of the body:
:
\mathbf = \mathrm(\mathbf)\mathbf - \mathbf

where covariance is defined as area integral over the triangle:
:
\mathbf \triangleq \int_ \rho \mathbf\mathbf^ = a \mathbf^ \mathbf

where
* \mathbf represents 3 × 3 matrix containing triangle vertex coordinates (\mathbf_0, \mathbf_1, \mathbf_2) in the rows,
* a = |(\mathbf_1 - \mathbf_0) \times (\mathbf_2 - \mathbf_0)| is twice the area of the triangle,
*
\mathbf= \frac
\begin
2 & 1 & 1 \\
1 & 2 & 1 \\
1 & 1 & 2 \\
\end

Substitution of triangle covariance in definition of inertia tensor gives eventually
:
\mathbf = \frac(\mathbf^2_0 + \mathbf^2_1 + \mathbf^2_2 + (\mathbf_0 + \mathbf_1 + \mathbf_2)^2)\mathbf - a \mathbf^ \mathbf

== A proof of the formula ==

The proof given here follows the steps from the article.〔http://number-none.com/blow/inertia/bb_inertia.doc Jonathan Blow, Atman J Binstock (2004)
"How to find the inertia tensor (or other mass properties) of a 3D solid body represented by a triangle mesh"〕

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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