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Exercise 840Calculus › Single-variable calculus › Differentiation › Taylor expansionsL2Added 3 Nov 2026

A fast series for ln 2

#logarithm#series#numerical approximation#speed of convergence

Statement

  1. Expand ln⁡1+t1−t\ln\frac{1+t}{1-t} at 00 up to order 55.
  2. Take t=13t=\frac13 to approximate ln⁡2\ln2, and bound the error.
  3. Compare with the plain expansion of ln⁡(1+x)\ln(1+x) at x=1x=1.
Hint

Subtract the expansions of ln⁡(1+t)\ln(1+t) and ln⁡(1−t)\ln(1-t): the even terms cancel.

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Solution

1. ln⁡(1+t)−ln⁡(1−t)=2(t+t33+t55+o(t5))\ln(1+t)-\ln(1-t)=2\left(t+\frac{t^3}3+\frac{t^5}5+o(t^5)\right).

2. For t=13t=\frac13: 1+t1−t=2\frac{1+t}{1-t}=2, so
ln⁡2≈2(13+181+11215)=0.69300…\ln2\approx2\left(\frac13+\frac1{81}+\frac1{1215}\right)=0.69300\ldots
The full series 2∑k≥0t2k+12k+12\sum_{k\ge0}\frac{t^{2k+1}}{2k+1} has positive terms, and the tail after k=2k=2 is bounded by a geometric series:
0<error<2⋅t77⋅11−t2=27⋅2187⋅98<1.5⋅10−4.0<\text{error}<2\cdot\frac{t^7}7\cdot\frac1{1-t^2}=\frac2{7\cdot2187}\cdot\frac98<1.5\cdot10^{-4}.
So 0.6930≤ln⁡2≤0.69320.6930\le\ln2\le0.6932 (true value 0.693147…0.693147\dots).

3. The series ln⁡(1+x)=x−x22+⋯\ln(1+x)=x-\frac{x^2}2+\cdots at x=1x=1 gives the alternating harmonic series, whose error after nn terms is of order 1n\frac1n: reaching 10−410^{-4} would need about 10410^4 terms, against just 33 terms above.

Remark. Choosing the expansion variable cleverly (t=13t=\frac13 instead of x=1x=1) is what makes numerical computations of ln⁡\ln practical.