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  "body": "\n## Definition\n\nLet $k$ be a real number with $0 \\le k \\le 1$.\nThe *complete elliptic integral of the second kind* is\n$$E(k) = \\int_0^{\\pi/2} \\sqrt{1 - k^2 \\sin^2\\theta} \\, d\\theta = \\int_0^1 \\frac{\\sqrt{1 - k^2 t^2}}{\\sqrt{1 - t^2}} \\, dt.$$\nIt is the value at $\\varphi = \\pi/2$ of the incomplete [[elliptic integral|NXMCYGCB59]] $E(\\varphi, k)$ of the second kind.\nWith $k' = \\sqrt{1 - k^2}$ one writes $E'(k) = E(k')$.\n\n## Remarks\n\nExample: $E(0) = \\pi/2$, and $E(1) = \\int_0^{\\pi/2} \\cos\\theta \\, d\\theta = 1$.\nThe ellipse $x = a\\sin\\theta$, $y = b\\cos\\theta$ with $0 \u003c b \\le a$ has perimeter $4aE(e)$, where $e = \\sqrt{1 - b^2/a^2}$ is its eccentricity, because its arc length element is $a\\sqrt{1 - e^2\\sin^2\\theta}\\,d\\theta$.\nNon-example: for real $k \u003e 1$ the integrand $\\sqrt{1 - k^2\\sin^2\\theta}$ is not real for $\\theta$ near $\\pi/2$, so the formula does not define a real number there.\nSeries: $E(k) = \\frac{\\pi}{2}\\left(1 - \\sum_{n=1}^{\\infty} \\left(\\frac{(2n)!}{2^{2n}(n!)^2}\\right)^2 \\frac{k^{2n}}{2n - 1}\\right)$.\nSome authors write $E(m)$ with the parameter $m = k^2$.\n",
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