| If the convergence is sufficiently uniform (so the derivatives converge), we have |
| (d/dε)fn(-2 + ε/rn)|ε=0 = gn'(ε)|ε=0 = g'(ε)|ε=0 |
| By the chain rule, the equation becomes |
| ((d/dc)fn(c)|c=-2)⋅((d/dε)(-2 + ε/rn)|e=0) = g'(0). |
| Motivated by the slope of f3 at the 3-cycle midget cardioid center, we take |
| g'(0) = -1. |
| With this, we find |
| rn = -fn'(-2) |
| The relation |
| fn+1(c) = (fn(c))2 + c |
| implies |
| fn+1'(c) = 2⋅fn(c)⋅fn'(c) + 1. |
| Using |
| fn'(-2) = -4n/6 - 1/3, |
| for n > 1. Dropping the -1/3, small compared to the other term for large n, we take the scaling factor to be |
| rn = 4n/6. |
Return to Hurwitz-Robucci scaling.