Exponential function: Difference between revisions

From Citizendium
Jump to navigation Jump to search
imported>Dmitrii Kouznetsov
m (→‎References: formating)
mNo edit summary
 
(13 intermediate revisions by 4 users not shown)
Line 1: Line 1:
'''Exponential function''' or exp, can be defined as solution of differential equation
{{subpages}}
: <math> \exp^{\prime}(z)=\exp(z)</math>
The '''exponential function''' of <math>z</math>, denoted by <math> \exp(z)</math> or <font style="vertical-align:+10%;"><math>e^z</math></font>, can be defined as the solution of the differential equation
: <math> \exp^{\prime}(z)\equiv \frac{d e^z}{dz}=\exp(z)</math>
with the additional condition  
with the additional condition  
: <math> \exp(0)=1 </math>
: <math> \exp(0)=1.\, </math>


The study of the exponential function began with [[Leonhard Euler]] around 1730<ref>William Dunham, ''Euler, the Master of us all'', MAA (1999) ISBN 0-8835-328-0.  Pp.17-37.</ref>
The study of the exponential function began with [[Leonhard Euler]] around 1730.<ref>William Dunham, ''Euler, the Master of us all'', MAA (1999) ISBN 0-8835-328-0.  Pp. 17-37.</ref>
Since that time, it has had widely applications in technology and science; in particular, [[exponential growth]] is described with such functions.
Since that time, it has had wide applications in technology and science; in particular, [[exponential growth]] is described with such functions.


==Properties==
==Properties==
The exponential is an [[entire function]].  
The exponential is an [[entire function]].  


For any complex <math>p</math> and <math>q</math>, the basic property holds:
For any complex ''p'' and ''q'', the basic property holds:
: <math> \exp(a)~\exp(b)=\exp(a+b) </math>
: <math> \exp(a)~\exp(b)=\exp(a+b) </math>
   
   
Line 17: Line 18:
where <math>\mathbb{C}</math> means the set of [[complex number]]s.
where <math>\mathbb{C}</math> means the set of [[complex number]]s.
The series converges for any complex <math>z</math>. In particular, the series converges for any real value of the argument.
The series converges for any complex <math>z</math>. In particular, the series converges for any real value of the argument.
: <math>\exp(z)=\lim_{n\rightarrow \infty}\left(1+\frac{z}{n}\right)^n ~ \forall z\in \mathbb{C}</math>


==Inverse function==
==Inverse function==
Line 34: Line 37:
: <math>{\rm e}=\exp(1) \approx 2.71828 18284 59045 23536</math>
: <math>{\rm e}=\exp(1) \approx 2.71828 18284 59045 23536</math>


==Relation with [[sin]] and [[cos]] functions==
==Periodicity and relation with [[sin]] and [[cos]] functions==
Exponential is [[periodic function]]; the period is <math>2 \pi \mathrm i </math>:
: <math> \exp(z+2\pi \mathrm{i})=\exp(z)  ~  \forall z\in \mathbb{C} </math>
 
The exponential is related to the [[trigonometric function]]s [[sine]] and [[cosine]] by ''[[de Moivre]]'s formula'':
The exponential is related to the [[trigonometric function]]s [[sine]] and [[cosine]] by ''[[de Moivre]]'s formula'':


Line 41: Line 47:
==Generalization of exponential==
==Generalization of exponential==


[[Image:Sqrt(exp)(z).jpg|right|500px|thumb|<math>\exp^c(z)</math> in the complex <math>z</math> plane for some real values of <math>c</math>.]]
{{Image|Sqrt(exp)(z).jpg|right|500px|<math>\exp^c(z)</math> in the complex <math>z</math> plane for some real values of <math>c</math>.}}


[[Image:Expc.jpg|right|200px|thumb|<math>\exp^c(x)</math> versus <math>x</math> for some real values of <math>c</math>.]]
{{Image|Expc.jpg|right|200px|<math>\exp^c(x)</math> versus <math>x</math> for some real values of <math>c</math>.}}
The notation <math>\exp_b</math> is used for the exponential with scaled argument;
The notation <math>\exp_b</math> is used for the exponential with scaled argument;


: <math>\exp_b(z)=b^z=\exp(\log(b) z)</math>
: <math>\exp_b(z)=b^z=\exp\!\Big(\log(b)~ z\Big)</math>


Notation <math>\exp_b^c</math> is used for the iterated exponential:
Notation <math>\exp_b^c</math> is used for the iterated exponential:
: <math> \exp_b^0(z) =z </math>
: <math> \exp_b^0(z) =z </math>
: <math> \exp_b^1(z) =\exp_b(z) </math>
: <math> \exp_b^1(z) =\exp_b(z) </math>
: <math> \exp_b^2(z) =\exp_b(\exp_b(z) </math>
: <math> \exp_b^2(z) =\exp_b\!\Big (\exp_b(z)\Big) </math>
: <math> \exp_b^{c+1}(z) =\exp_b(\exp_b^c(z) </math>
: <math> \exp_b^{c+1}(z) =\exp_b\!\Big(\exp_b^c(z)\Big) </math>


For non-integer values of <math>c</math>, the iterated exponential can be defined as
For non-integer values of <math>c</math>, the iterated exponential can be defined as
:  <math> \exp_b^c(z) =  
:  <math> \exp_b^c(z) =  
\mathrm{sexp}_b\Big(c+
\mathrm{sexp}_b\!\Big(c+
{\mathrm{sexp}_b}^{-1}(z)\Big) </math>
{\mathrm{sexp}_b}^{-1}(z)\Big) </math>
where <math> \mathrm{sexp}_b(z) </math> is function <math>F</math> satisfying conditions
where <math> \mathrm{sexp}_b(z) </math> is function <math>F</math> satisfying conditions


:<math>F(z+1)=\exp_b(F(z))</math>
:<math>F(z+1)=\exp_b\!\Big(F(z)\Big)</math>
:<math>F(0)=1</math>
:<math>F(0)=1</math>
:<math>F(z)~ \mathrm{ ~is~ holomorphic~ and~ bounded~ at}~ |\Re(z)|<1</math>
:<math>F(z)~ \mathrm{ ~is~ holomorphic~ and~ bounded~ at}~ |\Re(z)|<1</math>
Line 67: Line 73:
: <math>F\Big(F^{-1}(z)\Big)=z</math>
: <math>F\Big(F^{-1}(z)\Big)=z</math>
and, within some range of values of <math>z</math>
and, within some range of values of <math>z</math>
: <math>F^{-1}\Big (F(z)\Big)=z</math>
: <math>F^{-1}\Big(F(z)\Big)=z</math>


If in the notation <math>\exp_b^c</math> the superscript is omitted, it is assumed to be unity; for example
If in the notation <math>\exp_b^c</math> the superscript is omitted, it is assumed to be unity; for example
<math>\exp_b^1=\exp_b</math>. If the suberscript is omitted, it is assumed to be <math>\mathrm{e}</math>, id est, <math>\exp^c=\exp_\mathrm{e}^c</math>
<math>\exp_b^1=\exp_b</math>. If the subscript is omitted, it is assumed to be <math>\mathrm{e}</math>, id est, <math>\exp^c=\exp_\mathrm{e}^c</math>
 
Function <math>f=\exp^c(z)</math> is shown in figure with levels of constant real part and levels of constant imaginary part. Levels
<math>\Re(f)=-3,-2,-1,0,1,2,3,4,5,6,7,8,9</math> and
<math>\Im(f)=-3,-2,-1,0,1,2,3,4,5,6,7,8,9,10,11,12,13,14</math> are drown with thick lines.
Red corresponds to a negative value of the real or the imaginaryt part, black corresponds to zero, and blue corresponds to the positeive values.
Levels <math>\Re(f)=-0.2, -0.4, -0.6, -0.8</math> are shown with thin red lines.
Levels <math>\Im(f)= 0.2,  0.4,  0.6,  0.8</math> are shown with thin green lines.
Levels <math>\Re(f)=\Re(L)</math> and
Levels <math>\Im(f)=\Im(L)</math> are marked with thick green lines, where <math>L\approx  0.31813150520476413 +1.3372357014306895~ \mathrm{i}</math> is [[fixed point]] of logarithm.
At non-integer values of <math>c</math>, <math>L</math> and <math>L^*</math> are [[branch point]]s of function <math>\exp^c</math>; in figure, the cut is placed parallel to the real axis. At <math>c<0</math> there is an additional cut which goes along the negative part of the real axis. In the figure, the cuts are marked with pink lines.
 
For real values of the argument, function <math> y=\exp^c(x)</math> is ploted in figure versus <math>x</math> for values
<math>c=0,\pm 0.1, \pm 0.5, \pm 0.9, \pm 1, \pm 2</math>.<br>
in [[programming languages]], inverse function of exp is called [[log]].


At non-integer values of <math>c</math>, the [[fixed point]]s of logarithm
For [[logarithm]] on base e, notation ln is also used. In particular,
<math>L\approx  0.31813150520476413 \pm 1.3372357014306895~ \mathrm{i}</math> are [[branch point]]s of function </math>\exp^c</math>; in figure, the cut is placed parallel to the real axis.
<math>\exp^{-1}(x)=\ln(x)</math>,
At <math>c<0</math> there is an additional cut which goes along the negative part of the real axis. In the figure, these cuts are marked with pink.
<math>\exp^{-2}(x)=\ln\big(\ln(x)\big)</math> and so on.


==References==
==References==
Line 82: Line 102:
<!--
<!--
* H.Kneser. ``Reelle analytische L\"osungen der Gleichung <math>\varphi(\varphi(x))=\mathrm{e}^{x}</math> und verwandter Funktionalgleichungen''. Journal f\"ur die reine und angewandte Mathematik, <b> 187</b> (1950), 56-67.
* H.Kneser. ``Reelle analytische L\"osungen der Gleichung <math>\varphi(\varphi(x))=\mathrm{e}^{x}</math> und verwandter Funktionalgleichungen''. Journal f\"ur die reine und angewandte Mathematik, <b> 187</b> (1950), 56-67.
!-->
!-->[[Category:Suggestion Bot Tag]]
[[Category:Functions]]
[[Category:Mathematica functions]]

Latest revision as of 16:00, 14 August 2024

This article is developing and not approved.
Main Article
Discussion
Related Articles  [?]
Bibliography  [?]
External Links  [?]
Citable Version  [?]
 
This editable Main Article is under development and subject to a disclaimer.

The exponential function of , denoted by or , can be defined as the solution of the differential equation

with the additional condition

The study of the exponential function began with Leonhard Euler around 1730.[1] Since that time, it has had wide applications in technology and science; in particular, exponential growth is described with such functions.

Properties

The exponential is an entire function.

For any complex p and q, the basic property holds:

The definition allows to calculate all the derivatives at zero; so, the Taylor expansion has the form

where means the set of complex numbers. The series converges for any complex . In particular, the series converges for any real value of the argument.

Inverse function

The inverse function of the exponential is the logarithm; for any complex , the relation holds:

Exponential also can be considered as inverse of logarithm, while the imaginary part of the argument is smaller than :

When the logarithm has a cut along the negative part of the real axis, exp can be considered.

Number e

is widely used in applications; this notation is commonly accepted. Its approximate value is

Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle {\rm e}=\exp(1) \approx 2.71828 18284 59045 23536}

Periodicity and relation with sin and cos functions

Exponential is periodic function; the period is :

The exponential is related to the trigonometric functions sine and cosine by de Moivre's formula:

Generalization of exponential

(CC) Image: Dmitrii Kouznetsov
in the complex plane for some real values of .
(CC) Image: Dmitrii Kouznetsov
versus for some real values of .

The notation is used for the exponential with scaled argument;

Notation is used for the iterated exponential:

For non-integer values of , the iterated exponential can be defined as

where is function satisfying conditions

The inverse function is defined with condition

and, within some range of values of

If in the notation the superscript is omitted, it is assumed to be unity; for example . If the subscript is omitted, it is assumed to be , id est,

Function is shown in figure with levels of constant real part and levels of constant imaginary part. Levels and are drown with thick lines. Red corresponds to a negative value of the real or the imaginaryt part, black corresponds to zero, and blue corresponds to the positeive values. Levels are shown with thin red lines. Levels are shown with thin green lines. Levels and Levels are marked with thick green lines, where is fixed point of logarithm. At non-integer values of , and are branch points of function ; in figure, the cut is placed parallel to the real axis. At there is an additional cut which goes along the negative part of the real axis. In the figure, the cuts are marked with pink lines.

For real values of the argument, function is ploted in figure versus for values .
in programming languages, inverse function of exp is called log.

For logarithm on base e, notation ln is also used. In particular, , and so on.

References

  1. William Dunham, Euler, the Master of us all, MAA (1999) ISBN 0-8835-328-0. Pp. 17-37.
  • Ahlfors, Lars V. (1953). Complex analysis. McGraw-Hill Book Company, Inc..
  • H.Kneser. ``Reelle analytische Losungen der Gleichung und verwandter Funktionalgleichungen. Journal fur die reine und angewandte Mathematik, 187 (1950), 56-67.