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In mathematics, the Dottie number is a constant that is the unique real root of the equation
- ,
where the argument of is in radians.
The decimal expansion of the Dottie number is .[1]
Since is decreasing and its derivative is non-zero at , it only crosses zero at one point. This implies that the equation has only one real solution. It is the single real-valued fixed point of the cosine function and is a nontrivial example of a universal attracting fixed point. It is also a transcendental number because of the Lindemann-Weierstrass theorem.[2] The generalised case for a complex variable has infinitely many roots, but unlike the Dottie number, they are not attracting fixed points.
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Using the Taylor series of the inverse of at (or equivalently, the Lagrange inversion theorem), the Dottie number can be expressed as the infinite series where each is a rational number defined for odd n as[3][4][5][nb 1]
The name of the constant originates from a professor of French named Dottie who observed the number by repeatedly pressing the cosine button on her calculator.[3]
If a calculator is set to take angles in degrees, the sequence of numbers will instead converge to ,[6] the root of .
The Dottie number, for which an exact series expansion can be obtained using the Faà di Bruno formula, has interesting connections with the Kepler and Bertrand's circle problems.[7]
Closed form
The Dottie number can be expressed as
where is the inverse regularized Beta function. This value can be obtained using Kepler's equation, along with other equivalent closed forms.[8]
In Microsoft Excel and LibreOffice Calc spreadsheets, the Dottie number can be expressed in closed form as SQRT(1-(2*BETA.INV(1/2,1/2,3/2)-1)^2)
. In the Mathematica computer algebra system, the Dottie number is Sqrt[1 - (2 InverseBetaRegularized[1/2, 1/2, 3/2] - 1)^2]
.
Integral representations
Dottie number can be represented as
Or as
Two more representations are given as follows
Notes
- ↑ Kaplan does not give an explicit formula for the terms of the series, which follows trivially from the Lagrange inversion theorem.
References
- ↑ Sloane, N. J. A. (ed.). "Sequence A003957". The On-Line Encyclopedia of Integer Sequences. OEIS Foundation.
- ↑ Eric W. Weisstein. "Dottie Number".
- 1 2 Kaplan, Samuel R (February 2007). "The Dottie Number" (PDF). Mathematics Magazine. 80: 73. doi:10.1080/0025570X.2007.11953455. S2CID 125871044. Retrieved 29 November 2017.
- ↑ "OEIS A302977 Numerators of the rational factor of Kaplan's series for the Dottie number". oeis.org. Retrieved 2019-05-26.
- ↑ "A306254 - OEIS". oeis.org. Retrieved 2019-07-22.
- ↑ Sloane, N. J. A. (ed.). "Sequence A330119". The On-Line Encyclopedia of Integer Sequences. OEIS Foundation.
- ↑ Pain, Jean-Christophe (2023). "An exact series expansion for the Dottie number". arXiv:2303.17962.
- ↑ Gaidash, Tyma (2022-02-23). "Why Dottie$=2\sqrt{I^{-1}_\frac12(\frac 12,\frac 32)-I^{-1}_\frac12(\frac 12,\frac 32)^2} = \sin^{-1}\big(1-2I^{-1}_\frac12(\frac 12,\frac 32)\big)$?". Math Stack Exchange. Retrieved 2023-08-11.
- ↑ N/A, Anixx (2015-03-04). "Explaining $\cos^\infty$". Math Stack Exchange. Retrieved 2024-01-14.
- ↑ N/A, Jam (2020-01-24). "Explaining $\cos^\infty$". Math Stack Exchange. Retrieved 2024-01-14.
External links
- Miller, T. H. (Feb 1890). "On the numerical values of the roots of the equation cosx = x". Proceedings of the Edinburgh Mathematical Society. 9: 80–83. doi:10.1017/S0013091500030868.
- Salov, Valerii (2012). "Inevitable Dottie Number. Iterals of cosine and sine". arXiv:1212.1027.
- Azarian, Mohammad K. (2008). "ON THE FIXED POINTS OF A FUNCTION AND THE FIXED POINTS OF ITS COMPOSITE FUNCTIONS" (PDF). International Journal of Pure and Applied Mathematics.