<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://en.formulasearchengine.com/w/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=87.254.72.193</id>
	<title>formulasearchengine - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://en.formulasearchengine.com/w/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=87.254.72.193"/>
	<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/wiki/Special:Contributions/87.254.72.193"/>
	<updated>2026-08-12T02:40:23Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.47.0-wmf.7</generator>
	<entry>
		<id>https://en.formulasearchengine.com/w/index.php?title=Logic_alphabet&amp;diff=17303</id>
		<title>Logic alphabet</title>
		<link rel="alternate" type="text/html" href="https://en.formulasearchengine.com/w/index.php?title=Logic_alphabet&amp;diff=17303"/>
		<updated>2013-10-08T04:28:02Z</updated>

		<summary type="html">&lt;p&gt;87.254.72.193: /* Significance */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{E (mathematical constant)}}&lt;br /&gt;
{{refimprove|date=December 2007}}&lt;br /&gt;
The [[mathematical constant]] [[E (mathematical constant)|{{math|&#039;&#039;e&#039;&#039;}}]] can be represented in a variety of ways as a [[real number]].  Since {{math|&#039;&#039;e&#039;&#039;}} is an [[irrational number]] (see [[proof that e is irrational]]), it cannot be represented as a [[fraction (mathematics)|fraction]], but it can be represented as a [[continued fraction]].  Using [[calculus]], {{math|&#039;&#039;e&#039;&#039;}} may also be represented as an [[infinite series]], [[infinite product]], or other sort of [[limit of a sequence]].&lt;br /&gt;
&lt;br /&gt;
==As a continued fraction==&lt;br /&gt;
&lt;br /&gt;
[[Leonhard Euler|Euler]] proved that the number {{math|&#039;&#039;e&#039;&#039;}} is represented as the infinite [[simple continued fraction]]&amp;lt;ref&amp;gt;{{cite web|url=http://www.maa.org/editorial/euler/How%20Euler%20Did%20It%2028%20e%20is%20irrational.pdf|title=How Euler Did It: Who proved &#039;&#039;e&#039;&#039; is Irrational?|last=Sandifer|first=Ed|date=Feb. 2006|publisher=MAA Online|accessdate=2010-06-18}}&amp;lt;/ref&amp;gt; {{OEIS|id=A003417}}:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e = [2; 1, \textbf{2}, 1, 1, \textbf{4}, 1, 1, \textbf{6}, 1, 1, \textbf{8}, 1, 1, \ldots, \textbf{2n}, 1, 1, \ldots]. \,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Its convergence can be tripled by allowing just one fractional number:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; e = [ 1 ; \textbf{0.5} , 12 , 5 , 28 , 9 , 44 , 13 , 60 , 17 , \ldots , \textbf{4(4n-1)} , \textbf{4n+1} , \ldots]. \,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Here are some infinite [[generalized continued fraction]] expansions of {{math|&#039;&#039;e&#039;&#039;}}. The second is generated from the first by a simple [[generalized continued fraction#The equivalence transformation|equivalence transformation]].&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
e= 2+\cfrac{1}{1+\cfrac{1}{2+\cfrac{2}{3+\cfrac{3}{4+\cfrac{4}{5+\ddots}}}}} = 2+\cfrac{2}{2+\cfrac{3}{3+\cfrac{4}{4+\cfrac{5}{5+\cfrac{6}{6+\ddots\,}}}}}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e = 2+\cfrac{1}{1+\cfrac{2}{5+\cfrac{1}{10+\cfrac{1}{14+\cfrac{1}{18+\ddots\,}}}}} = 1+\cfrac{2}{1+\cfrac{1}{6+\cfrac{1}{10+\cfrac{1}{14+\cfrac{1}{18+\ddots\,}}}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This last, equivalent to [1; 0.5, 12, 5, 28, 9, ...], is a special case of a general formula for the [[exponential function]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e^{x/y} = 1+\cfrac{2x} {2y-x+\cfrac{x^2} {6y+\cfrac{x^2} {10y+\cfrac{x^2} {14y+\cfrac{x^2} {18y+\ddots}}}}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==As an infinite series==&lt;br /&gt;
The number {{math|&#039;&#039;e&#039;&#039;}} can be expressed as the sum of the following [[infinite series]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e^x = \sum_{k=0}^\infty \frac{x^k}{k!} &amp;lt;/math&amp;gt; for any real number &#039;&#039;x&#039;&#039;.&lt;br /&gt;
&lt;br /&gt;
In the special case where &#039;&#039;x&#039;&#039;&amp;amp;nbsp;=&amp;amp;nbsp;1, or &amp;amp;minus;1, we have:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e = \sum_{k=0}^\infty \frac{1}{k!}&amp;lt;/math&amp;gt;,&amp;lt;ref&amp;gt;{{cite web|url=http://oakroadsystems.com/math/loglaws.htm|title=It’s the Law Too — the Laws of Logarithms|last=Brown|first=Stan|date=2006-08-27|publisher=Oak Road Systems|accessdate=2008-08-14}}&amp;lt;/ref&amp;gt; and&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e^{-1} = \sum_{k=0}^\infty \frac{(-1)^k}{k!}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Other series include the following:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e = \left [ \sum_{k=0}^\infty \frac{1-2k}{(2k)!} \right ]^{-1}&amp;lt;/math&amp;gt; &amp;lt;ref&amp;gt;Formulas 2–7: [[Harlan J. Brothers|H. J. Brothers]],  [http://www.brotherstechnology.com/docs/Improving_Convergence_(CMJ-2004-01).pdf Improving the convergence of Newton&#039;s series approximation for &#039;&#039;e&#039;&#039;],  &#039;&#039;The College Mathematics Journal&#039;&#039;, Vol. 35, No. 1, (2004),  pp. 34–39.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \frac{1}{2} \sum_{k=0}^\infty \frac{k+1}{k!}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  2 \sum_{k=0}^\infty \frac{k+1}{(2k+1)!}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =   \sum_{k=0}^\infty \frac{3-4k^2}{(2k+1)!}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =   \sum_{k=0}^\infty \frac{(3k)^2+1}{(3k)!}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =   \left [ \sum_{k=0}^\infty \frac{4k+3}{2^{2k+1}\,(2k+1)!} \right ]^2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \left [ -\frac{12}{\pi^2} \sum_{k=1}^\infty \frac{1}{k^2} \ \cos \left ( \frac{9}{k\pi+\sqrt{k^2\pi^2-9}} \right ) \right ]^{-1/3} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k^n}{B_n(k!)}&amp;lt;/math&amp;gt; where &amp;lt;math&amp;gt;B_n&amp;lt;/math&amp;gt; is the &amp;lt;math&amp;gt;n^{th}&amp;lt;/math&amp;gt; [[Bell number]]. Some few examples: (for &#039;&#039;n&#039;&#039;=1,2,3)&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k}{k!} = \sum_{k=1}^\infty \frac{1}{(k-1)!} = \sum_{k=0}^\infty \frac{1}{k!}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k^2}{2(k!)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k^3}{5(k!)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k^4}{15(k!)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k^5}{52(k!)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k^6}{203(k!)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e =  \sum_{k=1}^\infty \frac{k^7}{877(k!)}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==As an infinite product==&lt;br /&gt;
The number {{math|&#039;&#039;e&#039;&#039;}} is also given by several [[infinite product]] forms including [[Nick Pippenger|Pippenger]]&#039;s product&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; e= 2 \left ( \frac{2}{1} \right )^{1/2} \left ( \frac{2}{3}\; \frac{4}{3} \right )^{1/4} \left ( \frac{4}{5}\; \frac{6}{5}\; \frac{6}{7}\; \frac{8}{7} \right )^{1/8} \cdots &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and Guillera&#039;s product &amp;lt;ref&amp;gt;J. Sondow, [http://arxiv.org/abs/math/0401406 A faster product for pi and a new integral for ln pi/2,] &#039;&#039;Amer. Math. Monthly&#039;&#039; 112 (2005) 729–734.&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;J. Guillera and J. Sondow, [http://arxiv.org/abs/math.NT/0506319 Double integrals and infinite products for some classical constants via analytic continuations of Lerch&#039;s transcendent,]&#039;&#039;Ramanujan Journal&#039;&#039; 16 (2008), 247–270.&amp;lt;/ref&amp;gt;&lt;br /&gt;
:&amp;lt;math&amp;gt; e = \left ( \frac{2}{1} \right )^{1/1} \left (\frac{2^2}{1 \cdot 3} \right )^{1/2} \left (\frac{2^3 \cdot 4}{1 \cdot 3^3} \right )^{1/3} &lt;br /&gt;
\left (\frac{2^4 \cdot 4^4}{1 \cdot 3^6 \cdot 5} \right )^{1/4}  \cdots ,&amp;lt;/math&amp;gt;&lt;br /&gt;
where the &#039;&#039;n&#039;&#039;th factor is the &#039;&#039;n&#039;&#039;th root of the product&lt;br /&gt;
:&amp;lt;math&amp;gt;\prod_{k=0}^n (k+1)^{(-1)^{k+1}{n \choose k}},&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
as well as the infinite product&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; e = \frac{2\cdot 2^{(\ln(2)-1)^2} \cdots}{2^{\ln(2)-1}\cdot 2^{(\ln(2)-1)^3}\cdots }.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==As the limit of a sequence==&lt;br /&gt;
The number {{math|&#039;&#039;e&#039;&#039;}} is equal to the [[limit of a sequence|limit]] of several [[infinite sequences]]:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; e= \lim_{n \to \infty} n\cdot\left ( \frac{\sqrt{2 \pi n}}{n!} \right )^{1/n}   &amp;lt;/math&amp;gt; and&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt; e=\lim_{n \to \infty} \frac{n}{\sqrt[n]{n!}} &amp;lt;/math&amp;gt; (both by [[Stirling&#039;s formula]]).&lt;br /&gt;
&lt;br /&gt;
The symmetric limit,&amp;lt;ref&amp;gt;[[Harlan J. Brothers|H. J. Brothers]] and J. A. Knox,  [http://www.brotherstechnology.com/docs/Closed-Form_Approximations_(MI-1998-12).pdf New closed-form approximations to the Logarithmic Constant &#039;&#039;e&#039;&#039;,] &#039;&#039;The Mathematical Intelligencer&#039;&#039;, Vol. 20, No. 4, (1998), pp. 25–29.&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;{{cite web|url=http://ans.hsh.no/home/skk/Publications/Lobatto/PRIMUS_KHATTRI.pdf|title=From Lobatto Quadrature to the Euler constant e|last=Khattri|first=Sanjay}}&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e=\lim_{n \to \infty} \left [ \frac{(n+1)^{n+1}}{n^n}- \frac{n^n}{(n-1)^{n-1}} \right ]&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
may be obtained by manipulation of the basic limit definition of {{math|&#039;&#039;e&#039;&#039;}}. Another limit is&amp;lt;ref&amp;gt;S. M. Ruiz 1997&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e= \lim_{n \to \infty}(p_n \#)^{1/p_n} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt; p_n &amp;lt;/math&amp;gt; is the &#039;&#039;n&#039;&#039;th [[prime number|prime]] and &amp;lt;math&amp;gt; p_n \# &amp;lt;/math&amp;gt; is the [[primorial]] of the &#039;&#039;n&#039;&#039;th prime.&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e= \lim_{n \to \infty}n^{\pi(n)/n} &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt; \pi(n) &amp;lt;/math&amp;gt; is the prime counting function. This definition is a direct corollary of the [[prime number theorem]].&lt;br /&gt;
&lt;br /&gt;
Also:&lt;br /&gt;
:&amp;lt;math&amp;gt;e^x= \lim_{n \to \infty}\left (1+ \frac{x}{n} \right )^n.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In the special case that &amp;lt;math&amp;gt;x = 1&amp;lt;/math&amp;gt;, the result is the famous statement:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;e= \lim_{n \to \infty}\left (1+ \frac{1}{n} \right )^n.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
== In trigonometry ==&lt;br /&gt;
Trigonometrically, {{math|&#039;&#039;e&#039;&#039;}} can be written as the sum of two [[hyperbolic functions]]:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt;e = \sinh(1) + \cosh(1)\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Notes==&lt;br /&gt;
{{reflist}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Transcendental numbers]]&lt;br /&gt;
[[Category:Mathematical constants]]&lt;br /&gt;
[[Category:Exponentials]]&lt;br /&gt;
[[Category:Logarithms]]&lt;br /&gt;
[[Category:E (mathematical constant)]]&lt;/div&gt;</summary>
		<author><name>87.254.72.193</name></author>
	</entry>
</feed>