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  "body": "\n## Definition\n\nLet $U \\subseteq \\mathbb{R}^n$ be open, and let $f \\colon U \\to \\mathbb{R}$ be twice differentiable on $U$.\nThe Laplacian of $f$ is the function $\\Delta f \\colon U \\to \\mathbb{R}$,\n$$\\Delta f = \\operatorname{div}(\\nabla f) = \\nabla \\cdot \\nabla f,$$\nthe [[divergence|02NSMQVQWK]] of the [[gradient|0NS2QYVC4Y]] of $f$. It is also written $\\nabla^2 f$.\n\n## Remarks\n\nIn Cartesian coordinates, $\\Delta f$ is the [[sum of the unmixed second partial derivatives|05RCT1522R]] of $f$.\nThe operator $\\Delta$ is linear, and it maps functions of [[class C^k|0TCBZMEYGN]] to functions of class $C^{k-2}$ for $k \\ge 2$.\nLet $f$ be of class $C^2$, and let $\\bar{f}_r$ be the average of $f$ on the sphere of radius $r$ about $x$. Then $\\Delta f(x)$ is $2n$ times the limit of $(\\bar{f}_r - f(x)) / r^2$ as $r \\to 0$. So $\\Delta f(x) \u003e 0$ means that $f(x)$ is below its nearby averages.\nThe Laplacian appears in the heat equation $\\partial_t u = \\Delta u$, the wave equation and Laplace's equation $\\Delta u = 0$.\n\n## Explanations\n\n### L1 human\n\nThe Laplacian compares the value of a function at a point with its values nearby.\nIf $f$ at the point is lower than the average around it, the Laplacian is positive. If it is higher, the Laplacian is negative.\n",
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