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  "body": "\n## Definition\n\nLet $S \\subseteq \\R^3$ be a [[regular surface|6080X3FAD4]] with a smooth unit [[normal vector|0BJDQ2HBH1]] field $N$.\nLet $\\alpha \\colon I \\to S$ be a curve of class $C^2$ parametrised by [[arc length|00R1JDDV5X]] on an interval $I$.\nThe *geodesic curvature* of $\\alpha$ at $s \\in I$ is\n$$\\kappa_g(s) = \\ip{\\alpha''(s)}{N(\\alpha(s)) \\times \\alpha'(s)},$$\nwhere $\\times$ is the [[cross product|0SEDGXG9S3]].\nThe *normal curvature* of $\\alpha$ at $s$ is $\\kappa_n(s) = \\ip{\\alpha''(s)}{N(\\alpha(s))}$.\n\n## Remarks\n\nSince $\\alpha'$, $N \\times \\alpha'$ and $N$ form an orthonormal basis and $\\ip{\\alpha''}{\\alpha'} = 0$, one has $\\alpha'' = \\kappa_g \\, N \\times \\alpha' + \\kappa_n N$.\nSo $\\kappa^2 = \\kappa_g^2 + \\kappa_n^2$, where $\\kappa$ is the [[curvature|7JQS6VKFEZ]] of $\\alpha$ as a space curve.\nExample: on the unit sphere with the outer normal $N(p) = p$, a great circle $\\alpha$ satisfies $\\alpha'' = -\\alpha$, which is normal to the sphere, so $\\kappa_g = 0$.\nA circle of latitude at polar angle $\\varphi_0 \\in (0, \\pi)$ has $\\kappa = 1 / \\sin \\varphi_0$ and $\\abs{\\kappa_g} = \\abs{\\cot \\varphi_0}$.\nNon-example: for a curve that is not of unit speed, the formula above is not the geodesic curvature; one must first reparametrise by arc length.\nFor a curve in the $xy$-plane with $N = (0, 0, 1)$, the geodesic curvature is the signed curvature of the plane curve.\n",
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