This page unifies three approximation families around a reference point \(x_0\): (1) the classical differential Taylor series (rank 0, operator \(D_0^n\)), (2) a relative multiplicative (“Product Taylor”) series (rank 1, operator \(D_1^n\)), (3) a rank-2 logarithmic–exponential series (rank 2, operator \(D_2^n\)). We always write derivatives explicitly with both rank and degree.
Choose \(x_0\) inside the domain. Approximation quality depends on the notion of “closeness”:
— Rank 0: additive closeness via \(x-x_0\).
— Rank 1: relative closeness via \(x/x_0\).
— Rank 2: logarithmic closeness via \(\ln x/\ln x_0\) (equivalently \(\ln(\ln x)\)).
The classical Taylor series built from the standard differential operator. Rank+degree is written \(D_0^n\).
Here \(D_{0}^{0}f=f\), \(D_{0}^{1}f=df/dx\), \(D_{0}^{2}f=d^2f/dx^2\), etc.
A “product Taylor”: sum → product, minus → division. Built from successive relative derivatives of degree \(n\) at rank 1.
where \[ \left(D_{1}^{n}\ln f\right)(x_0) = \left.\left(\frac{d}{d\ln x}\right)^{n}\ln f(x)\right|_{x=x_0}. \]
Here the degree \(n\) is the differentiation order with respect to \(\ln x\).
We expand \(\ln f\) with respect to \(\ln x\) (additive), then map back to \(f\) (multiplicative). A negative exponent means division: \[ \left(\frac{x}{x_0}\right)^{-a}=\frac{1}{\left(\frac{x}{x_0}\right)^{a}}. \]
In rank 2, the effective variable is \(\ln(\ln x)\). We use a practical formulation that approximates \(\ln f(x)\) relative to \(\ln f(x_0)\), while the rank-2 derivative itself is defined through \(\ln(\ln f)\).
where \(\ln^{(2)}f=\ln(\ln f)\), and \[ \left(D_{2}^{n}\ln^{(2)} f\right)(x_0) = \left.\left(\frac{d}{d\,\ln(\ln x)}\right)^{n}\ln(\ln f(x))\right|_{x=x_0}. \]
Rank 2 measures closeness through \(\ln(\ln x)\), hence \(\ln x/\ln x_0\) appears naturally. Negative exponents again correspond to division.
The goal is structural reasoning: which series captures a function shape more efficiently. Assume \(x_0>1\) (e.g., \(x_0=10\)) and compare near \(x_0\).
Strongest: rank 1 (relative multiplicative). Since \(\ln f=p\ln x\), the scale structure is captured extremely efficiently.
Strongest: rank 1 — a special case of power law with \(p=\tfrac12\).
Depends on closeness notion:
rank 0: best for very small additive neighborhoods.
rank 1: useful when change is discussed in relative terms.
rank 2: can help across broader scales when \(\ln(\ln f)\) is well-defined.
Often strongest: rank 2 (when defined), since \(\ln x\) aligns with \(\ln(\ln x)\) scale.
Locally: rank 0 also works well if \(x-x_0\) is small.
Strongest: rank 0 (Taylor), provided \(x_0\) is safely away from the pole \(x=1/\alpha\). Singularities often control additive convergence radii.
Strongest: rank 0 locally, since oscillations are best captured additively. Rank 1 is usually less economical for non-scale-invariant oscillations.
Often strongest: rank 1 for relative changes because variation is scale-driven and slow. Rank 0 is also good locally but may require higher degree for the same accuracy over larger relative changes.