ABSTRACT
It is well known that an infinitely differentiable function f(x) can be expanded in a Taylor series around a point x0 in the interval where it is defined. This series has the form
f(x) ∼ ∞∑
cn(x − x0)n, (2.1)
where the coefficients cn are given by
cn = f (n)(x0)
n! , n = 1,2, . . . , f (n) =
dnf
dxn .