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  "body": "\n## Definition\n\nLet $O$ be a point of the [[Euclidean plane|0XW7V9ZZ05]] and let $r \u003e 0$.\nThe *inversion in the [[circle|060W5CBZP6]]* with center $O$ and radius $r$ sends each point $P \\ne O$ to the unique point $P'$ such that:\n\n1. $P'$ lies on the ray from $O$ through $P$;\n2. $\\abs{OP} \\cdot \\abs{OP'} = r^2$.\n\n## Remarks\n\nIn coordinates with $O$ at the origin, the inversion is $x \\mapsto r^2 x / \\norm{x}^2$.\nIn complex notation with center $0$, it is $z \\mapsto r^2 / \\bar{z}$.\nAdding a point $\\infty$ and setting $O \\mapsto \\infty$ and $\\infty \\mapsto O$ extends it to a bijection of the [[Riemann sphere|0J78KBPFZB]].\nIt is an [[involution|GP56NBN9RY]]: applying it twice gives the identity.\nThe same formula defines inversion in a sphere of $\\R^n$.\n\nExample: for the circle with center $(0, 0)$ and radius $1$, the point $P = (2, 0)$ goes to $P' = (1/2, 0)$.\nCheck: $P'$ lies on the ray from the origin through $P$, and $\\abs{OP} \\cdot \\abs{OP'} = 2 \\cdot \\frac{1}{2} = 1$.\n\nNon-example: the map $x \\mapsto -r^2 x / \\norm{x}^2$ satisfies clause 2 but sends $P$ to the opposite ray, so clause 1 fails.\n",
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