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  "body": "\n## Definition\n\nLet $D$ be an open subset of $\\mathbb{R} \\times \\mathbb{R}^n$ and let $f : D \\to \\mathbb{R}^n$ be continuous.\nLet $I$ be an open interval and let $\\gamma : I \\to \\mathbb{R}^n$ be a [[solution|04SW7WECS8]] of $x' = f(t, x)$ whose graph lies in $D$.\nThe solution $\\gamma$ is maximal if there is no solution $\\tilde{\\gamma} : \\tilde{I} \\to \\mathbb{R}^n$ on an open interval $\\tilde{I}$ with $I \\subsetneq \\tilde{I}$ and $\\tilde{\\gamma}(t) = \\gamma(t)$ for each $t \\in I$.\nThe interval $I$ of a maximal solution is its maximal interval of existence.\n\n## Remarks\n\nIf $f$ is locally Lipschitz in $x$, each [[initial value problem|075VBY4K4X]] $x(t_0) = x_0$ with $(t_0, x_0) \\in D$ has exactly one maximal solution. Each other solution of the problem is a restriction of it.\nThe maximal interval $(t_-, t_+)$ can depend on the initial value, and it can be smaller than $\\mathbb{R}$.\nIf $t_+ \u003c \\infty$, then $(t, \\gamma(t))$ leaves every compact subset of $D$ as $t \\to t_+$. For $D = \\mathbb{R} \\times \\mathbb{R}^n$, this means $\\|\\gamma(t)\\| \\to \\infty$. See [[blow-up in finite time|0E4GXX7SJP]].\n\n## Explanations\n\n### L1 human\n\nA maximal solution is a solution that we cannot continue any further.\nIts interval ends only where the solution runs away to infinity or to the edge of the domain of the field.\n",
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