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  "body": "\n## Definition\n\nLet $\\sigma \\in \\set{1, -1}$.\nThe *Kadomtsev–Petviashvili equation* is the [[partial differential equation|GC5BDZ6QBC]]\n$$\\partial_x \\big( u_t + 6 u u_x + u_{xxx} \\big) + 3 \\sigma u_{yy} = 0$$\nfor an unknown real function $u(x, y, t)$ of $(x, y) \\in \\R^2$ and $t \\in \\R$, where subscripts denote [[partial derivatives|09EGC6F8PT]].\nThe case $\\sigma = 1$ is called *KP-II* and the case $\\sigma = -1$ is called *KP-I*.\n\n## Remarks\n\nExample: let $v(x, t)$ be a solution of the [[Korteweg–De Vries equation|KTT75QC72Z]] $v_t + 6 v v_x + v_{xxx} = 0$, and put $u(x, y, t) = v(x, t)$.\nThen the bracket vanishes and $u_{yy} = 0$, so $u$ solves both KP-I and KP-II.\n\nNon-example: $u(x, y, t) = y^2$ is not a solution, because the first term is $0$ while $3 \\sigma u_{yy} = 6 \\sigma \\ne 0$.\n\nOther normalisations are used, for example $\\partial_x(u_t + u u_x + \\varepsilon^2 u_{xxx}) + \\lambda u_{yy} = 0$ with $\\lambda = \\pm 1$.\nThey reduce to the form above by scaling the variables, and the sign of the $u_{yy}$ term relative to the dispersive term decides between KP-I and KP-II.\n",
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