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  "body": "\n## Definition\n\nLet $\\Omega$ be an open set in $\\R^n$ and let $m \\ge 1$.\nA [[partial differential equation|GC5BDZ6QBC]] of [[order|E7JDFDPM1X]] $m$ in $\\Omega$ is *quasilinear* if it has the following form.\n$$\\sum_{\\abs{\\alpha} = m} a_\\alpha\\left(D^{m-1} u, \\dots, D u, u, x\\right) \\partial^\\alpha u + a_0\\left(D^{m-1} u, \\dots, D u, u, x\\right) = 0.$$\nHere the functions $a_\\alpha$ and $a_0$ are given.\nHere $\\alpha$ runs over [[multi-indices|0PJXBR6QA3]], and $D^j u$ denotes the collection of all partial derivatives of order $j$.\nSo the equation is affine in the derivatives of order $m$, and its coefficients depend at most on the derivatives of order less than $m$.\n\n## Remarks\n\nExample: the minimal surface equation $\\operatorname{div}\\left(\\nabla u / \\sqrt{1 + \\abs{\\nabla u}^2}\\right) = 0$ in two variables expands to $(1 + u_y^2) u_{xx} - 2 u_x u_y u_{xy} + (1 + u_x^2) u_{yy} = 0$.\nThe coefficients of $u_{xx}$, $u_{xy}$, $u_{yy}$ depend only on first derivatives, so it is quasilinear of order $2$.\nNon-example: the Monge–Ampère equation $u_{xx} u_{yy} - u_{xy}^2 = f(x, y)$ is not quasilinear, because it contains products of second derivatives; it is [[fully nonlinear|2D3N1ZJWBW]].\nEvery [[semilinear PDE|RCNY89A4NY]] is quasilinear.\nFor first-order equations, quasilinear means $\\sum_{i} a_i(u, x) \\partial_i u + a_0(u, x) = 0$.\n\n## Explanations\n\n### L1 human\n\nQuasilinear means linear in the highest derivatives, once the solution and its lower derivatives are frozen.\n",
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