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  "body": "\n## Definition\n\nLet $E \\subseteq \\mathbb{R}^3$ be a bounded Jordan measurable set with a continuous density $\\delta \\colon E \\to [0, \\infty)$, and let $L$ be a line in $\\mathbb{R}^3$.\nFor $x \\in E$, let $d_L(x)$ be the distance from $x$ to $L$.\nThe moment of inertia of $E$ about $L$ is\n$$I_L = \\iiint_E d_L(x)^2 \\, \\delta(x) \\, dV.$$\nIn particular, $I_z = \\iiint_E (x^2 + y^2) \\, \\delta(x, y, z) \\, dV$ is the moment of inertia about the $z$-axis.\n\n## Remarks\n\nFor a plane lamina $D \\subseteq \\mathbb{R}^2$, the moments of inertia about the coordinate axes are $I_x = \\iint_D y^2 \\delta \\, dA$ and $I_y = \\iint_D x^2 \\delta \\, dA$. These are [[double integrals|0NKBMFC18R]].\nFor a point mass $m$ at distance $r$ from the axis, the moment of inertia is $m r^2$.\nExample: a solid cylinder of radius $a$, height $h$ and constant density has mass $M = \\delta \\pi a^2 h$ and $I_z = \\delta \\int_0^h \\int_0^{2\\pi} \\int_0^a r^3 \\, dr \\, d\\theta \\, dz = \\tfrac{1}{2} M a^2$.\nFor rotation about $L$ with angular velocity $\\omega$, the kinetic energy is $\\tfrac{1}{2} I_L \\omega^2$.\n\n## Explanations\n\n### L1 human\n\nMass far from the axis is harder to set spinning than mass close to it.\nThe moment of inertia adds up all the mass, weighted by the square of its distance from the axis.\n",
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