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The decimal value of the [[natural logarithm]] of [[2 (number)|2]] {{OEIS|A002162}}
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is approximately
:<math>\ln 2 \approx 0.69314718055...</math>
as shown in the first line of the table below.
The logarithm in other bases is obtained with the [[Logarithmic identities|formula]]
:<math>\log_b 2 = \frac{\ln 2}{\ln b}.</math>
The [[Briggsian logarithm|common logarithm]] in particular is ({{OEIS2C|A007524}})
:<math>\log_{10} 2 \approx 0.301029995663981195.</math>
The inverse of this number is the [[binary logarithm]] of 10:
:<math> \log_2 10=1/\log_{10} 2 \approx 3.321928095</math> ({{OEIS2C|A020862}}).
{{Table
|type=class="wikitable"
|hdrs=number!!approximate natural logarithm!![[OEIS]]
|row1=[[2 (number)|2]] {{!!}} 0.693147180559945309417232121458 {{!!}} {{OEIS link|A002162}}
|row2=[[3 (number)|3]]{{!!}}1.09861228866810969139524523692{{!!}} {{OEIS link|A002391}}
|row3=[[4 (number)|4]]{{!!}}1.38629436111989061883446424292{{!!}} {{OEIS link|A016627}}
|row4=[[5 (number)|5]]{{!!}}1.60943791243410037460075933323{{!!}} {{OEIS link|A016628}}
|row5=[[6 (number)|6]]{{!!}}1.79175946922805500081247735838{{!!}} {{OEIS link|A016629}}
|row6=[[7 (number)|7]]{{!!}}1.94591014905531330510535274344{{!!}} {{OEIS link|A016630}}
|row7=[[8 (number)|8]]{{!!}}2.07944154167983592825169636437{{!!}} {{OEIS link|A016631}}
|row8=[[9 (number)|9]]{{!!}}2.19722457733621938279049047384{{!!}} {{OEIS link|A016632}}
|row9=[[10 (number)|10]]{{!!}}2.30258509299404568401799145468{{!!}} {{OEIS link|A002392}}
}}
 
==Series representations==
 
:<math>\sum_{n=1}^\infty \frac{(-1)^{n+1}}{n} = \sum_{n=0}^\infty \frac{1}{(2n+1)(2n+2)} = \ln 2.</math>
 
:<math>\sum_{n=1}^\infty \frac{(-1)^n}{(n+1)(n+2)} = 2\ln 2 -1.</math>
 
:<math>\sum_{n=1}^\infty \frac{1}{n(4n^2-1)} = 2\ln 2 -1.</math>
 
:<math>\sum_{n=1}^\infty \frac{(-1)^n}{n(4n^2-1)} = \ln 2 -1.</math>
 
:<math>\sum_{n=1}^\infty \frac{(-1)^n}{n(9n^2-1)} = 2\ln 2 -\frac{3}{2}.</math>
 
:<math>\sum_{n=2}^\infty \frac{1}{2^n}[\zeta(n)-1] = \ln 2 -\frac{1}{2}.</math>
 
:<math>\sum_{n=1}^\infty \frac{1}{2n+1}[\zeta(n)-1] = 1-\gamma-\frac{1}{2}\ln 2.</math>
 
:<math>\sum_{n=1}^\infty \frac{1}{2^{2n}(2n+1)}\zeta(2n) = \frac{1}{2}(1-\ln 2).</math>
 
:<math>\ln 2 = \sum_{k\ge 1} \frac{1}{k2^k}.</math>
 
:<math>\ln 2 = \sum_{k\ge 1}\left(\frac{1}{3^k}+\frac{1}{4^k}\right)\frac{1}{k}.</math>
 
:<math>\ln 2 = \frac{2}{3}+\sum_{k\ge 1}\left(\frac{1}{2k}+\frac{1}{4k+1}+\frac{1}{8k+4}+\frac{1}{16k+12}\right)\frac{1}{16^k}.</math>
 
:<math>\ln 2 = \frac{2}{3} \sum_{k\ge 0} \frac{1}{(2k+1)9^k}.</math>
 
(<math>\gamma</math> is the [[Euler constant|Euler–Mascheroni constant]]
and <math>\zeta</math> [[Riemann zeta function|Riemann's zeta function]]).
 
Some [[Bailey–Borwein–Plouffe formula|Bailey–Borwein–Plouffe (BBP)-type representations]] fall also into this category.
 
==Representation as integrals==
 
:<math>\int_0^1 \frac{dx}{1+x} = \ln 2,\text{ or, equivalently, }\int_1^2 \frac{dx}{x} = \ln 2.</math>
 
:<math>\int_1^\infty \frac{dx}{(1+x^2)(1+x)^2} = \frac{1}{4}(1-\ln 2).</math>
 
:<math>\int_0^\infty \frac{dx}{1+e^{nx}} = \frac{1}{n}\ln 2;
\int_0^\infty \frac{dx}{3+e^{nx}} = \frac{2}{3n}\ln 2.</math>
 
:<math>\int_0^\infty \frac{1}{e^x-1}-\frac{2}{e^{2x}-1}\,dx=\ln 2.</math>
 
:<math>\int_0^\infty e^{-x}\frac{1-e^{-x}}{x} \, dx= \ln 2.</math>
 
:<math>\int_0^1 \ln\frac{x^2-1}{x\ln x}dx=-1+\ln 2+\gamma.</math>
 
:<math>\int_0^{\pi/3} \tan x \, dx=2\int_0^{\pi/4} \tan x \, dx=\ln 2.</math>
 
:<math>\int_{-\pi/4}^{\pi/4} \ln(\sin x+\cos x)\,dx=-\frac{\pi}{4}\ln 2.</math>
 
:<math>\int_0^1 x^2\ln(1+x)\,dx=\frac{2}{3}\ln 2-\frac{5}{18}.</math>
 
:<math>\int_0^1 x\ln(1+x)\ln(1-x)\,dx=\frac{1}{4}-\ln 2.</math>
 
:<math>\int_0^1 x^3\ln(1+x)\ln(1-x)\,dx=\frac{13}{96}-\frac{2}{3}\ln 2.</math>
 
:<math>\int_0^1 \frac{\ln x}{(1+x)^2}\,dx = -\ln 2.</math>
 
:<math>\int_0^1 \frac{\ln(1+x)-x}{x^2}\,dx=1-2\ln2.</math>
 
:<math>\int_0^1 \frac{dx}{x(1-\ln x)(1-2\ln x)} = \ln 2.</math>
 
:<math>\int_1^\infty \frac{\ln\ln x}{x^3}\,dx = -\frac{1}{2}(\gamma+\ln 2).</math>
 
(<math>\gamma</math> is the [[Euler constant|Euler–Mascheroni constant]]).
 
==Other representations==
The Pierce expansion is {{OEIS2C|A091846}}
:<math> \ln 2 = \frac{1}{1} -\frac{1}{1\cdot 3}+\frac{1}{1\cdot 3\cdot 12} -\cdots. </math>
The [[Engel expansion]] is {{OEIS2C|A059180}}
:<math> \ln 2 = \frac{1}{2} + \frac{1}{2\cdot 3} + \frac{1}{2\cdot 3\cdot 7} + \frac{1}{2\cdot 3\cdot 7\cdot 9}+\cdots. </math>
The cotangent expansion is {{OEIS2C|A081785}}
:<math> \ln 2 = \cot (\operatorname{arccot} 0 -\operatorname{arccot} 1 + \operatorname{arccot} 5 - \operatorname{arccot} 55 + \operatorname{arccot} 14187 -\cdots). </math>
As an infinite sum of fractions:<ref>"The Penguin's Dictionary of Curious and Interesting Numbers" by David Wells, page 29.</ref>
:<math> \ln 2 = \frac{1}{1} -\frac{1}{2} +\frac{1}{3} -\frac{1}{4} +\frac{1}{5} -\cdots. </math>
This [[generalized continued fraction]]:
:<math> \ln 2 = \left[ 0;1,2,3,1,5,\frac{2}{3},7,\frac{1}{2},9,\frac{2}{5},...,2k-1,\frac{2}{k},...\right] </math>,<ref>[http://www.kurims.kyoto-u.ac.jp/EMIS/journals/EM/expmath/volumes/13/13.3/BorweinCrandallFee.pdf On the Ramanujan AGM Fraction, I: The Real-Parameter Case. Experimental Mathematics, Vol. 13 (2004), No. 3, pages 278,280.]</ref>
:also expressible as
:<math> \ln 2 = \cfrac{1} {1+\cfrac{1} {2+\cfrac{1} {3+\cfrac{2} {2+\cfrac{2} {5+\cfrac{3} {2+\cfrac{3} {7+\cfrac{4} {2+\ddots}}}}}}}}
= \cfrac{2} {3-\cfrac{1^2} {9-\cfrac{2^2} {15-\cfrac{3^2} {21-\ddots}}}} </math>
 
==Bootstrapping other logarithms==
Given a value of <math>\ln 2</math>, a scheme of computing the
logarithms of other [[integer]]s is to tabulate the logarithms of the
[[prime number]]s and in the next layer the logarithms of the [[Composite number|composite]]
numbers <math>c</math> based on their [[Table of prime factors|factorizations]]
:<math>c=2^i3^j5^k7^\ell\cdots\rightarrow \ln c=i\ln 2+j\ln 3+k\ln 5+\ell\ln 7+\cdots</math>
 
Apart from the logarithms of 2, 3, 5 and 7 shown above, this employs
{{Table
|type=class="wikitable sortabel"
|hdrs=prime!!approximate natural logarithm!![[OEIS]]
|row1=[[11 (number)|11]] {{!!}} 2.39789527279837054406194357797 {{!!}} {{OEIS link|A016634}}
|row2=[[13 (number)|13]] {{!!}} 2.56494935746153673605348744157 {{!!}} {{OEIS link|A016636}}
|row3=[[17 (number)|17]] {{!!}} 2.83321334405621608024953461787 {{!!}} {{OEIS link|A016640}}
|row4=[[19 (number)|19]] {{!!}} 2.94443897916644046000902743189 {{!!}} {{OEIS link|A016642}}
|row5=[[23 (number)|23]] {{!!}} 3.13549421592914969080675283181 {{!!}} {{OEIS link|A016646}}
|row6=[[29 (number)|29]] {{!!}} 3.36729582998647402718327203236 {{!!}} {{OEIS link|A016652}}
|row7=[[31 (number)|31]] {{!!}} 3.43398720448514624592916432454 {{!!}} {{OEIS link|A016654}}
|row8=[[37 (number)|37]] {{!!}} 3.61091791264422444436809567103 {{!!}} {{OEIS link|A016660}}
|row9=[[41 (number)|41]] {{!!}} 3.71357206670430780386676337304 {{!!}} {{OEIS link|A016664}}
|row10=[[43 (number)|43]] {{!!}} 3.76120011569356242347284251335 {{!!}} {{OEIS link|A016666}}
|row11=[[47 (number)|47]] {{!!}} 3.85014760171005858682095066977 {{!!}} {{OEIS link|A016670}}
|row12=[[53 (number)|53]] {{!!}} 3.97029191355212183414446913903 {{!!}} {{OEIS link|A016676}}
|row13=[[59 (number)|59]] {{!!}} 4.07753744390571945061605037372 {{!!}} {{OEIS link|A016682}}
|row14=[[61 (number)|61]] {{!!}} 4.11087386417331124875138910343 {{!!}} {{OEIS link|A016684}}
|row15=[[67 (number)|67]] {{!!}} 4.20469261939096605967007199636 {{!!}} {{OEIS link|A016690}}
|row16=[[71 (number)|71]] {{!!}} 4.26267987704131542132945453251 {{!!}} {{OEIS link|A016694}}
|row17=[[73 (number)|73]] {{!!}} 4.29045944114839112909210885744 {{!!}} {{OEIS link|A016696}}
|row18=[[79 (number)|79]] {{!!}} 4.36944785246702149417294554148 {{!!}} {{OEIS link|A016702}}
|row19=[[83 (number)|83]] {{!!}} 4.41884060779659792347547222329 {{!!}} {{OEIS link|A016706}}
|row20=[[89 (number)|89]] {{!!}} 4.48863636973213983831781554067 {{!!}} {{OEIS link|A016712}}
|row21=[[97 (number)|97]] {{!!}} 4.57471097850338282211672162170 {{!!}} {{OEIS link|A016720}}
}}
 
In a third layer, the logarithms of rational numbers <math>r=a/b</math>
are computed with <math>\ln r = \ln a -\ln b</math>, and logarithms of roots
via <math>\ln \sqrt[n]{c} = \frac{1}{n}\ln c</math>.
 
The logarithm of [[2 (number)|2]] is useful in the sense that the powers
of 2 are rather densely distributed; finding powers <math>2^i</math>
close to powers <math>b^j</math> of other numbers <math>b</math> is
comparatively easy, and series representations of <math>\ln b</math>
are found by coupling <math>2</math> to <math>b</math>
with [[Logarithmic identities|logarithmic conversions]].
 
===Example===
If <math>p^s=q^t+d</math> with some small <math>d</math>,
then <math>p^s/q^t=1+d/q^t</math> and therefore
:<math> s\ln p-t\ln q = \ln\left(1+\frac{d}{q^t}\right) =
\sum_{m=1}^\infty (-1)^{m+1}\frac{(d/q^t)^m}{m}.
</math>
Selecting <math>q=2</math>
represents <math>\ln p</math> by <math>\ln 2</math> and a series of
a parameter <math>d/q^t</math> that one wishes to keep small for quick convergence. Taking <math>3^2=2^3+1</math>, for example, generates
:<math> 2\ln 3 = 3\ln 2-\sum_{k\ge 1}\frac{(-1)^k}{k8^k}.</math>
This is actually the third line in the following table of
expansions of this type:
<!--
:<math> 5\ln 3 = 8\ln 2-\sum_{k\ge 1}\frac{1}{k}(\frac{13}{256})^k.</math>
:<math> 6\ln 5 = 14\ln 2-\sum_{k\ge 1}\frac{1}{k}(\frac{759}{16384})^k.</math>
:<math> \ln 7 = 3\ln 2-\sum_{k\ge 1}\frac{1}{k8^k}.</math>
:<math> 5\ln 7 = 14\ln 2-\sum_{k\ge 1}\frac{(-1)^k}{k}(\frac{423}{16384})^k.</math>
:<math> \ln 17 = 4\ln 2-\sum_{k\ge 1}\frac{(-1)^k}{k16^k}.</math>
-->
{{Table
|type=class="wikitable sortable"
|hdrs=s!!p!!t!!q!!d/q<sup>''t''</sup>
|row1=1{{!!}}3 {{!!}} 1 {{!!}} 2 {{!!}} 1 / 2 = 0.50000000...
|row2=1{{!!}}3 {{!!}} 2 {{!!}} 2 {{!!}} −1 / 4 = −0.25000000...
|row3=2{{!!}}3 {{!!}} 3 {{!!}} 2 {{!!}} 1 / 8 = 0.12500000...
|row4=5{{!!}}3 {{!!}} 8 {{!!}} 2 {{!!}} −13 / 256 = −0.05078125...
|row5=12{{!!}}3 {{!!}} 19 {{!!}} 2 {{!!}} 7153 / 524288 = 0.01364326...
|row6=1{{!!}}5 {{!!}} 2 {{!!}} 2 {{!!}} 1 / 4 = 0.25000000...
|row7=3{{!!}}5 {{!!}} 7 {{!!}} 2 {{!!}} −3 / 128 = −0.02343750...
|row8=1{{!!}}7 {{!!}} 2 {{!!}} 2 {{!!}} 3 / 4 = 0.75000000...
|row9=1{{!!}}7 {{!!}} 3 {{!!}} 2 {{!!}} −1 / 8 = −0.12500000...
|row10=5{{!!}}7 {{!!}} 14 {{!!}} 2 {{!!}} 423 / 16384 = 0.02581787...
|row11=1{{!!}}11 {{!!}} 3 {{!!}} 2 {{!!}} 3 / 8 = 0.37500000...
|row12=2{{!!}}11 {{!!}} 7 {{!!}} 2 {{!!}} −7 / 128 = −0.05468750...
|row13=11{{!!}}11 {{!!}} 38 {{!!}} 2 {{!!}} 10433763667 / 274877906944 = 0.03795781...
|row14=1{{!!}}13 {{!!}} 3 {{!!}} 2 {{!!}} 5 / 8 = 0.62500000...
|row15=1{{!!}}13 {{!!}} 4 {{!!}} 2 {{!!}} −3 / 16 = −0.18750000...
|row16=3{{!!}}13 {{!!}} 11 {{!!}} 2 {{!!}} 149 / 2048 = 0.07275391...
|row17=7{{!!}}13 {{!!}} 26 {{!!}} 2 {{!!}} −4360347 / 67108864 = −0.06497423...
|row18=10{{!!}}13 {{!!}} 37 {{!!}} 2 {{!!}} 419538377 / 137438953472 = 0.00305254...
|row19=1{{!!}}17 {{!!}} 4 {{!!}} 2 {{!!}} 1 / 16 = 0.06250000...
|row20=1{{!!}}19 {{!!}} 4 {{!!}} 2 {{!!}} 3 / 16 = 0.18750000...
|row21=4{{!!}}19 {{!!}} 17 {{!!}} 2 {{!!}} −751 / 131072 = −0.00572968...
|row22=1{{!!}}23 {{!!}} 4 {{!!}} 2 {{!!}} 7 / 16 = 0.43750000...
|row23=1{{!!}}23 {{!!}} 5 {{!!}} 2 {{!!}} −9 / 32 = −0.28125000...
|row24=2{{!!}}23 {{!!}} 9 {{!!}} 2 {{!!}} 17 / 512 = 0.03320312...
|row25=1{{!!}}29 {{!!}} 4 {{!!}} 2 {{!!}} 13 / 16 = 0.81250000...
|row26=1{{!!}}29 {{!!}} 5 {{!!}} 2 {{!!}} −3 / 32 = −0.09375000...
|row27=7{{!!}}29 {{!!}} 34 {{!!}} 2 {{!!}} 70007125 / 17179869184 = 0.00407495...
|row28=1{{!!}}31 {{!!}} 5 {{!!}} 2 {{!!}} −1 / 32 = −0.03125000...
|row29=1{{!!}}37 {{!!}} 5 {{!!}} 2 {{!!}} 5 / 32 = 0.15625000...
|row30=4{{!!}}37 {{!!}} 21 {{!!}} 2 {{!!}} −222991 / 2097152 = −0.10633039...
|row31=5{{!!}}37 {{!!}} 26 {{!!}} 2 {{!!}} 2235093 / 67108864 = 0.03330548...
|row32=1{{!!}}41 {{!!}} 5 {{!!}} 2 {{!!}} 9 / 32 = 0.28125000...
|row33=2{{!!}}41 {{!!}} 11 {{!!}} 2 {{!!}} −367 / 2048 = −0.17919922...
|row34=3{{!!}}41 {{!!}} 16 {{!!}} 2 {{!!}} 3385 / 65536 = 0.05165100...
|row35=1{{!!}}43 {{!!}} 5 {{!!}} 2 {{!!}} 11 / 32 = 0.34375000...
|row36=2{{!!}}43 {{!!}} 11 {{!!}} 2 {{!!}} −199 / 2048 = −0.09716797...
|row37=5{{!!}}43 {{!!}} 27 {{!!}} 2 {{!!}} 12790715 / 134217728 = 0.09529825...
|row38=7{{!!}}43 {{!!}} 38 {{!!}} 2 {{!!}} −3059295837 / 274877906944 = −0.01112965...
 
}}
 
Starting from the natural logarithm of <math>q=10</math> one might use these parameters:
{{Table
|type=class="wikitable sortable"
|hdrs=s!!p!!t!!q!!d/q<sup>''t''</sup>
|row1=10{{!!}}2 {{!!}} 3 {{!!}} 10 {{!!}} 3 / 125 = 0.02400000...
|row2=21{{!!}}3 {{!!}} 10 {{!!}} 10 {{!!}} 460353203 / 10000000000 = 0.04603532...
|row3=3{{!!}}5 {{!!}} 2 {{!!}} 10 {{!!}} 1 / 4 = 0.25000000...
|row4=10{{!!}}5 {{!!}} 7 {{!!}} 10 {{!!}} −3 / 128 = −0.02343750...
|row5=6{{!!}}7 {{!!}} 5 {{!!}} 10 {{!!}} 17649 / 100000 = 0.17649000...
|row6=13{{!!}}7 {{!!}} 11 {{!!}} 10 {{!!}} −3110989593 / 100000000000 = −0.03110990...
|row7=1{{!!}}11 {{!!}} 1 {{!!}} 10 {{!!}} 1 / 10 = 0.10000000...
|row8=1{{!!}}13 {{!!}} 1 {{!!}} 10 {{!!}} 3 / 10 = 0.30000000...
|row9=8{{!!}}13 {{!!}} 9 {{!!}} 10 {{!!}} −184269279 / 1000000000 = −0.18426928...
|row10=9{{!!}}13 {{!!}} 10 {{!!}} 10 {{!!}} 604499373 / 10000000000 = 0.06044994...
|row11=1{{!!}}17 {{!!}} 1 {{!!}} 10 {{!!}} 7 / 10 = 0.70000000...
|row12=4{{!!}}17 {{!!}} 5 {{!!}} 10 {{!!}} −16479 / 100000 = −0.16479000...
|row13=9{{!!}}17 {{!!}} 11 {{!!}} 10 {{!!}} 18587876497 / 100000000000 = 0.18587876...
|row14=3{{!!}}19 {{!!}} 4 {{!!}} 10 {{!!}} −3141 / 10000 = −0.31410000...
|row15=4{{!!}}19 {{!!}} 5 {{!!}} 10 {{!!}} 30321 / 100000 = 0.30321000...
|row16=7{{!!}}19 {{!!}} 9 {{!!}} 10 {{!!}} −106128261 / 1000000000 = −0.10612826...
|row17=2{{!!}}23 {{!!}} 3 {{!!}} 10 {{!!}} −471 / 1000 = −0.47100000...
|row18=3{{!!}}23 {{!!}} 4 {{!!}} 10 {{!!}} 2167 / 10000 = 0.21670000...
|row19=2{{!!}}29 {{!!}} 3 {{!!}} 10 {{!!}} −159 / 1000 = −0.15900000...
|row20=2{{!!}}31 {{!!}} 3 {{!!}} 10 {{!!}} −39 / 1000 = −0.03900000...
 
}}
 
==References==
* {{cite journal
|first1=Richard P.
|last1=Brent
|title=Fast multiple-precision evaluation of elementary functions
|journal=J. ACM
|volume=23
|issue=2
|year=1976
|pages=242&ndash;251
|doi=10.1145/321941.321944
|mr=0395314
}}
* {{cite journal
|first1=Horace S.
|last1=Uhler
|title=Recalculation and extension of the modulus and of the logarithms of 2, 3, 5, 7 and 17
|journal=Proc. Natl. Acad. Sci. U.S.A.
|volume=26
|year=1940
|pages=205&ndash;212
|url=http://www.pnas.org/content/26/3/205.full.pdf+html
|mr=0001523
}}
* {{cite journal
|first1=Dura W.
|last1=Sweeney
|title=On the computation of Euler's constant
|journal=Mathematics of Computation
|year=1963
|volume=17
|pages=170-178
|doi=10.1090/S0025-5718-1963-0160308-X
|mr=0160308
}}
* {{cite journal
|first1=Marc
|last1=Chamberland
|title=Binary BBP-formulae for logarithms and generalized Gaussian–Mersenne primes
|journal=Journal of Integer Sequences
|url=http://www.emis.ams.org/journals/JIS/VOL6/Chamberland/chamberland60.pdf
|volume=6
|page=03.3.7
|year=2003
|mr=2046407
}}
* {{cite journal
|first1=Boris
|last1=Gour&eacute;vitch
|first2=Jesus
|last2=Guillera Goyanes
|title=Construction of binomial sums for &pi; and polylogarithmic constants inspired by BBP formulas
|journal=Applied Math. E-Notes
|volume=7
|year=2007
|url=http://www.math.nthu.edu.tw/~amen/2007/061028-2.pdf
|mr=2346048
|pages=237&ndash;246}}
* {{cite journal
|first1=Qiang
|last1=Wu
|title=On the linear independence measure of logarithms of rational numbers
|journal=Mathematics of Computation
|volume=72
|issue=242
|pages=901&ndash;911
|doi=10.1090/S0025-5718-02-01442-4
|year=2003
}}
{{reflist}}
 
==External links==
* {{MathWorld|urlname=NaturalLogarithmof2|title=Natural logarithm of 2}}
* {{planetmath reference|id=10699|title=table of natural logarithms}}
 
* {{cite web|url=http://numbers.computation.free.fr/Constants/Log2/log2.html|title=The logarithm constant:log 2|last1=Gourdon|first1=Xavier|last2=Sebah|first2=Pascal}}
 
{{DEFAULTSORT:Natural Logarithm Of 2}}
[[Category:Numbers]]
[[Category:Logarithms]]
[[Category:Irrational numbers]]

Latest revision as of 14:31, 25 September 2014

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Our test subjects had been average-sized thirteen year-old boys. The wristband match comfortably on the wrist for both boys. After a few hours, one boy complained it was too unfastened and finally made his own gap additional up the band along with his pocket knife. Each boys said they observed the yellow plastic grommet however neither were bothered by it. The wristband match snugly on the boys' ankles and in both instances, came unfastened while they performed within the lake. Both boys said the band felt no different than any other gel bracelet they're accustomed to wearing. "It just smelled better," one boy declared.