Using this we can find g(e) with a lot of combinatorics of the taylor series, or we can
recall the trigonometric identity
g(e) = 2cos(sqrt(e))
satisfies g(4e) = g(e)2 - 2.
g(4e) = 2cos(sqrt(4e)) = 2cos(2sqrt(e)) = 2(2cos2(sqrt(e)) - 1) = g(e)2 - 2
Here is an anmiation illustrating the convergence of gn(e) to g(e).
|
| Click the picture to animate. |
Return to Hurwitz-Robucci scaling.