A381254 Decimal expansion of the obliquity (in radians) of a planet at which the annual instellations received by the poles and the equator are identical.
9, 4, 0, 6, 6, 6, 7, 7, 0, 2, 3, 9, 9, 9, 9, 6, 6, 3, 2, 1, 5, 8, 8, 1, 8, 6, 7, 9, 9, 3, 8, 5, 7, 9, 0, 5, 3, 2, 8, 8, 2, 0, 5, 4, 7, 1, 7, 1, 6, 9, 0, 5, 6, 4, 6, 8, 5, 0, 5, 4, 7, 1, 2, 0, 1, 2, 7, 4, 6, 7, 1, 4, 1, 3, 7, 7, 7, 8, 8, 7, 0, 7, 3, 4, 3, 7, 6, 7, 0, 3, 2, 1, 6, 3, 0, 8, 0, 7, 2, 4, 3, 4, 4, 7
Offset: 0
Examples
0.9406667702399996632...
Links
- David Ferreira, John Marshall, Paul A. O’Gorman, and Sara Seager, Climate at high-obliquity Icarus, vol. 243, pp. 236-248, 2014.
- John Marshall, Climate at high-obliquity
- D. M. Williams, J. F. Kasting, and L. A. Frakes, Low-latitude glaciation and rapid changes in the Earth's obliquity explained by obliquity-oblateness feedback, Nature, 1998 Dec 3;396(6710):453-5.
- Worldbuilding Pasta, Climate Explorations: Obliquity
Crossrefs
Cf. A383141.
Programs
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Mathematica
FindRoot[(EllipticE[Sin[x]^2] + Sqrt[Cos[x]^2] * EllipticE[-Tan[x]^2]) / Pi == Sin[x], {x, 0.94}, WorkingPrecision -> 100]
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PARI
\\ definition of ellM as in Mathematica's EllipticE[m] ellM(k) = intnum(t=0, Pi/2, sqrt(1-k*sin(t)^2)); solve (x=0.9, 0.95, (ellM(sin(x)^2) + sqrt(cos(x)^2)*ellM(-tan(x)^2))/Pi - sin(x)) \\ Hugo Pfoertner, Apr 26 2025
Formula
Equals A383141*Pi/180.
Comments