Exponential function: Difference between revisions
Jump to navigation
Jump to search
→Relationship with trigonometry: Added a step in the derivation of complex exponentiation |
imported>Spiral6800 m Add skin-invert-image class |
||
| Line 4: | Line 4: | ||
{{Infobox mathematical function | {{Infobox mathematical function | ||
| name = Exponential | | name = Exponential | ||
| image = Image:exp.svg | | image = Image:exp.svg{{!}}class=skin-invert-image | ||
| imagealt = Graph of the exponential function | | imagealt = Graph of the exponential function | ||
| caption = Graph of the exponential function | | caption = Graph of the exponential function | ||
| Line 18: | Line 18: | ||
| reciprocal = <math>\exp(-z)</math> | | reciprocal = <math>\exp(-z)</math> | ||
| inverse = [[Natural logarithm]], [[Complex logarithm]] | | inverse = [[Natural logarithm]], [[Complex logarithm]] | ||
| derivative = <math>\ | | derivative = <math>\frac{\mathrm{d}}{\mathrm{d}\!\,z} \exp z = \exp z</math> | ||
| antiderivative = <math>\int \exp z\,dz = \exp z + C</math> | | antiderivative = <math>\int \exp z\,dz = \exp z + C</math> | ||
| taylor_series = <math>\exp z = \sum_{n=0}^\infty\frac{z^n}{n!}</math> | | taylor_series = <math>\exp z = \sum_{n=0}^\infty\frac{z^n}{n!}</math> | ||
}} | }} | ||
In [[mathematics]], the '''exponential function''' is the unique [[real function]] which maps [[0|zero]] to [[1|one]] and has a [[ | In [[mathematics]], the '''exponential function''' is the unique [[real function]] which maps [[0|zero]] to [[1|one]] and has a [[derivative]] everywhere equal to its value. It is denoted {{tmath|e^x}} or {{tmath|\exp x}}; the latter is preferred when the argument {{tmath|x}} is a complicated expression.<ref>{{cite web |title=Reviews of Modern Physics Style Guide |url=https://cdn.journals.aps.org/files/rmpguide.pdf |publisher=American Physical Society |access-date=30 December 2025 |location=XVI.B.1(d) |page=18 |quote=Which form to use, {{tmath|e}} or {{tmath|\exp}}, is determined by the number of characters and the complexity of the argument. The {{tmath|e}} form is appropriate when the argument is short and simple, i.e., <math>e^{i \mathbf{k}\cdot\mathbf{r}}</math>, whereas {{tmath|\exp}} should be used if the argument is more complicated.}}</ref><ref>{{cite book |author1=T. W. Chaundy |author2=P. R. Barrett |author3=Charles Batey |title=The Printing of Mathematics |date=1954 |publisher=Oxford University Press |page=31 |url=https://archive.org/details/printingofmathem0000chau/page/31/}}</ref> It is called ''exponential'' because its argument can be seen as an [[exponent (mathematics)|exponent]] to which a constant [[e (mathematical constant)|number {{math|''e'' ≈ 2.718}}]], the base, is raised. There are several other definitions of the exponential function, which are all equivalent although being of very different nature. | ||
The exponential function converts sums to products: | The exponential function converts sums to products: {{tmath|1=\exp(x + y) = \exp x \cdot \exp y }}. Its [[inverse function]], the [[natural logarithm]], {{tmath|\ln}} or {{tmath|\log}}, converts products to sums: {{tmath|1= \ln(x\cdot y) = \ln x + \ln y}}. | ||
The exponential function is occasionally called the '''natural exponential function''', matching the name ''natural logarithm'', for distinguishing it from some other functions that are also commonly called ''exponential functions''. These functions include the functions of the form {{tmath|1=f(x) = b^x}}, which is [[exponentiation]] with a fixed base {{tmath|b}}. More generally, and especially in applications, functions of the general form {{tmath|1=f(x) = ab^x}} are also called exponential functions. They [[exponential growth|grow]] or [[exponential decay|decay]] exponentially in that the rate that {{tmath|f(x)}} changes when {{tmath|x}} is increased is ''proportional'' to the current value of {{tmath|f(x)}}. | The exponential function is occasionally called the '''natural exponential function''', matching the name ''natural logarithm'', for distinguishing it from some other functions that are also commonly called ''exponential functions''. These functions include the functions of the form {{tmath|1=f(x) = b^x}}, which is [[exponentiation]] with a fixed base {{tmath|b}}. More generally, and especially in applications, functions of the general form {{tmath|1=f(x) = ab^x}} are also called exponential functions. They [[exponential growth|grow]] or [[exponential decay|decay]] exponentially in that the rate that {{tmath|f(x)}} changes when {{tmath|x}} is increased is ''proportional'' to the current value of {{tmath|f(x)}}. | ||
The exponential function can be generalized to accept [[complex number]]s as arguments. This reveals relations between multiplication of complex numbers, rotations in the [[complex plane]], and [[trigonometry]]. [[Euler's formula]] {{tmath|1= | The exponential function can be generalized to accept [[complex number]]s as arguments. This reveals relations between multiplication of complex numbers, rotations in the [[complex plane]], and [[trigonometry]]. [[Euler's formula]] {{tmath|1= e^{i\theta} = \cos\theta + i\sin\theta}} expresses and summarizes these relations. | ||
The exponential function can be even further generalized to accept other types of arguments, such as [[Matrix exponentiation|matrices]] and elements of [[Exponential map (Lie theory)|Lie algebras]]. | The exponential function can be even further generalized to accept other types of arguments, such as [[Matrix exponentiation|matrices]] and elements of [[Exponential map (Lie theory)|Lie algebras]]. | ||
| Line 43: | Line 43: | ||
[[Image:Exp tangent.svg|thumb|right |The derivative of the exponential function is equal to the value of the function. Since the derivative is the [[slope]] of the tangent, this implies that all green [[right triangle]]s have a base length of 1.]] | [[Image:Exp tangent.svg|thumb|right |The derivative of the exponential function is equal to the value of the function. Since the derivative is the [[slope]] of the tangent, this implies that all green [[right triangle]]s have a base length of 1.]] | ||
The exponential function is the unique [[differentiable function]] that equals its [[derivative]], and takes the value {{math|1}} for the value {{math|0}} of its variable. | |||
This | This definition requires a uniqueness proof and an existence proof, but it allows an easy derivation of the main properties of the exponential function. | ||
===Inverse of natural logarithm=== | ===Inverse of natural logarithm=== | ||
The exponential function is the [[inverse function]] of the [[natural logarithm]]. That is, | |||
:<math>\begin{align} | :<math>\begin{align} | ||
\ln (\exp x)&=x\\ | \ln (\exp x)&=x\\ | ||
| Line 60: | Line 56: | ||
===Power series=== | ===Power series=== | ||
The exponential function is the sum of the [[power series]]<ref name="Rudin_1987"/><ref name=":0">{{Cite web|last=Weisstein| first=Eric W.|title=Exponential Function|url=https://mathworld.wolfram.com/ExponentialFunction.html|access-date=2020-08-28| website=mathworld.wolfram.com|language=en}}</ref> | |||
<math display=block> | <math display=block> | ||
\begin{align}\exp(x) &= 1+x+\frac{x^2}{2!}+ \frac{x^3}{3!}+\cdots\\ | \begin{align}\exp(x) &= 1+x+\frac{x^2}{2!}+ \frac{x^3}{3!}+\cdots\\ | ||
&=\sum_{n=0}^\infty \frac{x^n}{n!},\end{align}</math> | &=\sum_{n=0}^\infty \frac{x^n}{n!},\end{align}</math> | ||
[[Image:Exp series.gif|right|thumb|The exponential function (in blue), and the sum of the first {{math|''n'' + 1}} terms of its power series (in red)]] | [[Image:Exp series.gif|right|thumb|The exponential function (in blue), and the sum of the first {{math|''n'' + 1}} terms of its power series (in red)]] | ||
where <math>n!</math> is the [[factorial]] of {{mvar|n}} (the product of the {{mvar|n}} first positive integers). This series is [[absolutely convergent]] for every <math>x</math> | where <math>n!</math> is the [[factorial]] of {{mvar|n}} (the product of the {{mvar|n}} first positive integers). This series is [[absolutely convergent]] for every <math>x</math>, by the [[ratio test]]. This shows that the exponential function is defined for every {{tmath|x}}, and is everywhere the sum of its [[Maclaurin series]]. | ||
===Functional equation=== | ===Functional equation=== | ||
The exponential satisfies the [[functional equation]] | |||
<math display=block>\exp(x+y)= \exp(x)\cdot \exp(y) | <math display=block>\exp(x+y)= \exp(x)\cdot \exp(y)</math> | ||
and maps the [[additive identity]] {{math|0}} to the [[multiplicative identity]] {{math|1}}. | |||
<math> f(x)= | The same equation is satisfied by other continuous functions <math>f(x)=b^x</math> that exponentiate their argument with an arbitrary base <math>b</math>.<ref>{{cite book | ||
| last = Jung | first = Soon-Mo | |||
| contribution = Chapter 9: Exponential Functional Equations | |||
| doi = 10.1007/978-1-4419-9637-4_9 | |||
| isbn = 9781441996374 | |||
| series = Springer Optimization and Its Applications | |||
| pages = 207–225 | |||
| publisher = Springer New York | |||
| title = Hyers-Ulam-Rassias Stability of Functional Equations in Nonlinear Analysis | |||
| year = 2011 | |||
| volume = 48 | |||
}}</ref> Among these functions, the exponential function is characterized by the property that its derivative at {{math|0}} is {{math|1}}.<ref>{{cite book | |||
| last1 = Aczél | first1 = J. | |||
| last2 = Dhombres | first2 = J. | |||
| doi = 10.1017/CBO9781139086578 | |||
| isbn = 0-521-35276-2 | |||
| mr = 1004465 | |||
| page = 10 | |||
| publisher = Cambridge University Press, Cambridge | |||
| series = Encyclopedia of Mathematics and its Applications | |||
| title = Functional Equations in Several Variables | |||
| volume = 31 | |||
| year = 1989}}</ref> | |||
===Limit of integer powers=== | ===Limit of integer powers=== | ||
The exponential function is the [[limit (mathematics)|limit]], as the integer {{mvar|n}} goes to infinity,<ref name="Maor"/><ref name=":0" /> | |||
<math display=block>\exp(x)=\lim_{n \to +\infty} \left(1+\frac xn\right)^n.</math> | <math display=block>\exp(x)=\lim_{n \to +\infty} \left(1+\frac xn\right)^n.</math> | ||
===Properties=== | ===Properties=== | ||
| Line 89: | Line 101: | ||
''Positiveness:'' {{tmath|e^x>0}} for every real number {{tmath|x}}. This results from the [[intermediate value theorem]], since {{tmath|1=e^0=1}} and, if one would have {{tmath|e^x<0}} for some {{tmath|x}}, there would be an {{tmath|y}} such that {{tmath|1=e^y=0}} between {{tmath|0}} and {{tmath|x}}. Since the exponential function equals its derivative, this implies that the exponential function is [[monotonically increasing]]. | ''Positiveness:'' {{tmath|e^x>0}} for every real number {{tmath|x}}. This results from the [[intermediate value theorem]], since {{tmath|1=e^0=1}} and, if one would have {{tmath|e^x<0}} for some {{tmath|x}}, there would be an {{tmath|y}} such that {{tmath|1=e^y=0}} between {{tmath|0}} and {{tmath|x}}. Since the exponential function equals its derivative, this implies that the exponential function is [[monotonically increasing]]. | ||
''Extension of [[exponentiation]] to positive real bases:'' Let {{mvar|b}} be a positive real number. The exponential function | ''Extension of [[exponentiation]] to positive real bases:'' Let {{mvar|b}} be a positive real number. The exponential function and the natural logarithm being the inverse each of the other, one has <math>b=\exp(\ln b).</math> If {{mvar|n}} is an integer, the functional equation of the logarithm implies | ||
<math display=block>b^n=\exp(\ln b^n)= \exp(n\ln b).</math> | <math display=block>b^n=\exp(\ln b^n)= \exp(n\ln b).</math> | ||
Since the right-most expression is defined if {{mvar|n}} is any real number, this allows defining {{tmath|b^x}} for every positive real number {{mvar|b}} and every real number {{mvar|x}}: | Since the right-most expression is defined if {{mvar|n}} is any real number, this allows defining {{tmath|b^x}} for every positive real number {{mvar|b}} and every real number {{mvar|x}}: | ||
| Line 109: | Line 121: | ||
[[Image:Exponenciala priklad.png|thumb|200px|right|Exponential functions with bases 2 and 1/2]] | [[Image:Exponenciala priklad.png|thumb|200px|right|Exponential functions with bases 2 and 1/2]] | ||
The ''base'' of an exponential function | The ''base'' of an exponential function is the ''base'' of the [[exponentiation]] that appears in it when written as {{tmath|x\to ab^x}}, namely {{tmath|b}}.<ref>G. Harnett, ''Calculus 1'', 1998; Functions continued / Exponentials & logarithms: "The ratio of outputs for a unit change in input is the ''base'' of a general exponential function."</ref> The base is {{tmath|e^k}} in the second characterization, <math display=inline>\exp \frac{f'(x)}{f(x)}</math> in the third one, and <math display=inline>\left(\frac{f(x+d)}{f(x)}\right)^{1/d}</math> in the last one. | ||
===In applications=== | ===In applications=== | ||
The last characterization is important in [[empirical science]]s, as allowing a direct [[experimental]] test whether a function is an exponential function. | The last characterization is important in [[empirical science]]s, as allowing a direct [[experimental]] test whether a function is an exponential function. | ||
Exponential [[exponential growth|growth]] or [[exponential decay]]{{mdash}}where the variable change is [[proportionality (mathematics)|proportional]] to the variable value{{mdash}}are thus modeled with exponential functions. Examples are unlimited population growth leading to [[Malthusian catastrophe]], [[compound interest#Continuous compounding|continuously compounded interest]], and [[radioactive decay]]. | Exponential [[exponential growth|growth]] or [[exponential decay]]{{mdash}}where the variable change is [[proportionality (mathematics)|proportional]] to the variable value{{mdash}}are thus modeled with exponential functions. Examples are unlimited population growth leading to [[Malthusian catastrophe]], [[compound interest#Continuous compounding|continuously compounded interest]], and [[radioactive decay]]. | ||
| Line 127: | Line 139: | ||
Suppose that the third condition is verified, and let {{tmath|k}} be the constant value of <math>f'(x)/f(x).</math> Since <math display = inline>\frac {\partial e^{kx}}{\partial x}=ke^{kx},</math> the [[quotient rule]] for derivation | Suppose that the third condition is verified, and let {{tmath|k}} be the constant value of <math>f'(x)/f(x).</math> Since <math display = inline>\frac {\partial e^{kx}}{\partial x}=ke^{kx},</math> the [[quotient rule]] for derivation | ||
implies that | implies that | ||
<math display=block>\frac \partial{\partial x}\,\frac{f(x)}{e^{kx}}=0,</math> and thus that there is a constant {{tmath|a}} such that <math>f(x)=ae^{kx}.</math> | <math display=block>\frac \partial{\partial x}\,\frac{f(x)}{e^{kx}}=0,</math> and thus that there is a constant {{tmath|a}} such that <math>f(x)=ae^{kx}.</math> | ||
If the last condition is verified, let <math display=inline>\varphi(d)=f(x+d)/f(x),</math> which is independent of {{tmath|x}}. Using {{tmath|1=\varphi (0)=1}}, one gets | If the last condition is verified, let <math display=inline>\varphi(d)=f(x+d)/f(x),</math> which is independent of {{tmath|x}}. Using {{tmath|1=\varphi (0)=1}}, one gets | ||
| Line 158: | Line 170: | ||
involve exponential functions in a more sophisticated way, since they have the form | involve exponential functions in a more sophisticated way, since they have the form | ||
<math display=block>y=ce^{-kx}+e^{-kx}\int f(x)e^{kx}dx,</math> | <math display=block>y=ce^{-kx}+e^{-kx}\int f(x)e^{kx}dx,</math> | ||
where {{tmath|c}} is an arbitrary constant and the integral denotes any [[antiderivative]] of its argument. | where {{tmath|c}} is an arbitrary constant and the integral denotes any [[antiderivative]] of its argument. | ||
More generally, the solutions of every linear differential equation with constant coefficients can be expressed in terms of exponential functions and, when they are not homogeneous, antiderivatives. This holds true also for systems of linear differential equations with constant coefficients. | More generally, the solutions of every linear differential equation with constant coefficients can be expressed in terms of exponential functions and, when they are not homogeneous, antiderivatives. This holds true also for systems of linear differential equations with constant coefficients. | ||
==Complex exponential== | == Complex exponential == | ||
{{anchor|On the complex plane|Complex plane}} | {{anchor|On the complex plane|Complex plane}} | ||
[[File:The exponential function e^z plotted in the complex plane from -2-2i to 2+2i.svg|alt=The exponential function {{math|''e''{{isup|''z''}}}} plotted in the complex plane from {{math|−2 − 2''i''}} to {{math|2 + 2''i''}}|thumb|The exponential function {{math|''e''{{isup|''z''}}}} plotted in the complex plane from {{math|−2 − 2''i''}} to {{math|2 + 2''i''}}]] | [[File:The exponential function e^z plotted in the complex plane from -2-2i to 2+2i.svg|alt=The exponential function {{math|''e''{{isup|''z''}}}} plotted in the complex plane from {{math|−2 − 2''i''}} to {{math|2 + 2''i''}}|thumb|The exponential function {{math|''e''{{isup|''z''}}}} plotted in the complex plane from {{math|−2 − 2''i''}} to {{math|2 + 2''i''}}]] | ||
[[Image:Exp-complex-cplot.svg|thumb|right|A [[Domain coloring|complex plot]] of <math>z\mapsto\exp z</math>, with the [[Argument (complex analysis)|argument]] <math>\operatorname{Arg}\exp z</math> represented by varying hue. The transition from dark to light colors shows that <math>\left|\exp z\right|</math> is increasing only to the right. The periodic horizontal bands corresponding to the same hue indicate that <math>z\mapsto\exp z</math> is [[periodic function|periodic]] in the [[imaginary part]] of <math>z</math>.]] | [[Image:Exp-complex-cplot.svg|thumb|right|A [[Domain coloring|complex plot]] of <math>z\mapsto\exp z</math>, with the [[Argument (complex analysis)|argument]] <math>\operatorname{Arg}\exp z</math> represented by varying hue. The transition from dark to light colors shows that <math>\left|\exp z\right|</math> is increasing only to the right. The periodic horizontal bands corresponding to the same hue indicate that <math>z\mapsto\exp z</math> is [[periodic function|periodic]] in the [[imaginary part]] of <math>z</math>.]] | ||
The exponential function can be naturally extended to a [[complex function]], which is a function with the [[complex number]]s as | The exponential function can be naturally extended to a [[complex function]], which is a function with the [[complex number]]s as [[domain of a function|domain]] and [[codomain]], such that its [[restriction (mathematics)|restriction]] to the reals is the above-defined exponential function, called ''real exponential function'' in what follows. This function is also called ''the exponential function'', and also denoted {{tmath|e^z}} or {{tmath|\exp(z)}}. For distinguishing the complex case from the real one, the extended function is also called '''complex exponential function''' or simply '''complex exponential'''. | ||
Most of the definitions of the exponential function can be used verbatim for definiting the complex exponential function, and the proof of their equivalence is the same as in the real case. | Most of the definitions of the exponential function can be used verbatim for definiting the complex exponential function, and the proof of their equivalence is the same as in the real case. | ||
The complex exponential function can be defined | The complex exponential function can be defined in several equivalent ways that are the same as in the real case. | ||
The ''complex exponential'' is the unique complex function that equals its [[complex derivative]] and takes the value {{tmath|1}} for the argument {{tmath|0}}: | The ''complex exponential'' is the unique complex function that equals its [[complex derivative]] and takes the value {{tmath|1}} for the argument {{tmath|0}}: | ||
| Line 178: | Line 190: | ||
The ''complex exponential function'' is the sum of the [[series (mathematics)|series]] | The ''complex exponential function'' is the sum of the [[series (mathematics)|series]] | ||
<math display="block">e^z = \sum_{k = 0}^\infty\frac{z^k}{k!}.</math> | <math display="block">e^z = \sum_{k = 0}^\infty\frac{z^k}{k!}.</math> | ||
This series is [[absolutely convergent]] for every complex number {{tmath|z}}. So, the complex | This series is [[absolutely convergent]] for every complex number {{tmath|z}}. So, the complex exponential is an [[entire function]]. | ||
The complex exponential function is the [[limit (mathematics)|limit]] | The complex exponential function is the [[limit (mathematics)|limit]] | ||
<math display="block">e^z = \lim_{n\to\infty}\left(1+\frac{z}{n}\right)^n</math> | <math display="block">e^z = \lim_{n\to\infty}\left(1+\frac{z}{n}\right)^n</math> | ||
As with the real exponential function (see {{section link||Functional equation}} above), the complex exponential satisfies the functional equation | |||
<math display= | <math display=block>\exp(z+w)= \exp(z)\cdot \exp(w).</math> | ||
Among complex functions, it is the unique solution which is [[holomorphic]] at the point {{tmath|1= z = 0}} and takes the derivative {{tmath|1}} there.<ref>{{cite book |last=Hille |first=Einar |year=1959 |title=Analytic Function Theory |volume=1 |place=Waltham, MA |publisher=Blaisdell |chapter=The exponential function |at=§ 6.1, {{pgs|138–143}} }}</ref> | |||
The [[complex logarithm]] is a [[left inverse function|right-inverse function ]] of the complex exponential: | The [[complex logarithm]] is a [[left inverse function|right-inverse function]] of the complex exponential: | ||
<math display="block">e^{\log z} =z. </math> | <math display="block">e^{\log z} =z. </math> | ||
However, since the complex logarithm is a [[multivalued function]], one has | However, since the complex logarithm is a [[multivalued function]], one has | ||
| Line 197: | Line 209: | ||
and | and | ||
<math display="block">e^z\neq 0\quad \text{for every } z\in \C .</math> | <math display="block">e^z\neq 0\quad \text{for every } z\in \C .</math> | ||
It is [[ | It is [[periodic function]] of period {{tmath|2i\pi}}; that is | ||
<math display="block">e^{z+2ik\pi} =e^z \quad \text{for every } k\in \Z.</math> | <math display="block">e^{z+2ik\pi} =e^z \quad \text{for every } k\in \Z.</math> | ||
This results from [[Euler's identity]] {{tmath|1=e^{i\pi}=-1}} and the functional identity. | This results from [[Euler's identity]] {{tmath|1=e^{i\pi}=-1}} and the functional identity. | ||
| Line 204: | Line 216: | ||
<math display="block">\overline{e^z}=e^{\overline z}.</math> | <math display="block">\overline{e^z}=e^{\overline z}.</math> | ||
Its modulus is | Its modulus is | ||
<math display="block">|e^z|= e^{ | <math display="block">|e^z|= e^{\Re (z)},</math> | ||
where {{tmath|\Re(z)}} denotes the real part of {{tmath|z}}. | where {{tmath|\Re(z)}} denotes the real part of {{tmath|z}}. | ||
| Line 223: | Line 235: | ||
In these formulas, {{tmath|x, y, t}} are commonly interpreted as real variables, but the formulas remain valid if the variables are interpreted as complex variables. These formulas may be used to define trigonometric functions of a complex variable.<ref name="Apostol_1974"/> | In these formulas, {{tmath|x, y, t}} are commonly interpreted as real variables, but the formulas remain valid if the variables are interpreted as complex variables. These formulas may be used to define trigonometric functions of a complex variable.<ref name="Apostol_1974"/> | ||
===Plots=== | === Plots === | ||
<gallery caption="3D plots of real part, imaginary part, and modulus of the exponential function" class="center" mode="packed" style="text-align:left" heights="150px"> | <gallery caption="3D plots of real part, imaginary part, and modulus of the exponential function" class="center" mode="packed" style="text-align:left" heights="150px"> | ||
| Line 238: | Line 250: | ||
<gallery class="center" mode="packed" style="text-align:left" heights="200px" caption="Graphs of the complex exponential function"> | <gallery class="center" mode="packed" style="text-align:left" heights="200px" caption="Graphs of the complex exponential function"> | ||
File: Complex exponential function graph domain xy dimensions.svg|Checker board key: | File: Complex exponential function graph domain xy dimensions.svg|Checker board key:{{br}} <math>x> 0:\; \text{green}</math>{{br}} <math>x< 0:\; \text{red}</math>{{br}}<math>y> 0:\; \text{yellow}</math>{{br}}<math>y< 0:\; \text{blue}</math> | ||
File: Complex exponential function graph range vw dimensions.svg|Projection onto the range complex plane (V/W). Compare to the next, perspective picture. | File: Complex exponential function graph range vw dimensions.svg|Projection onto the range complex plane (V/W). Compare to the next, perspective picture. | ||
File: Complex exponential function graph horn shape xvw dimensions.jpg|Projection into the <math>x</math>, <math>v</math>, and <math>w</math> dimensions, producing a flared horn or funnel shape (envisioned as 2-D perspective image)|alt=Projection into the <nowiki> </nowiki> x <nowiki> </nowiki> {\displaystyle x} , <nowiki> </nowiki> v <nowiki> </nowiki> {\displaystyle v} , and <nowiki> </nowiki> w <nowiki> </nowiki> {\displaystyle w} <nowiki> </nowiki>dimensions, producing a flared horn or funnel shape (envisioned as 2-D perspective image). | File: Complex exponential function graph horn shape xvw dimensions.jpg|Projection into the <math>x</math>, <math>v</math>, and <math>w</math> dimensions, producing a flared horn or funnel shape (envisioned as 2-D perspective image)|alt=Projection into the <nowiki> </nowiki> x <nowiki> </nowiki> {\displaystyle x} , <nowiki> </nowiki> v <nowiki> </nowiki> {\displaystyle v} , and <nowiki> </nowiki> w <nowiki> </nowiki> {\displaystyle w} <nowiki> </nowiki>dimensions, producing a flared horn or funnel shape (envisioned as 2-D perspective image). | ||
File: Complex exponential function graph spiral shape yvw dimensions.jpg|Projection into the <math>y</math>, <math>v</math>, and <math>w</math> dimensions, producing a spiral shape (<math>y</math> range extended to ±2{{pi}}, again as | File: Complex exponential function graph spiral shape yvw dimensions.jpg|Projection into the <math>y</math>, <math>v</math>, and <math>w</math> dimensions, producing a spiral shape (<math>y</math> range extended to ±2{{pi}}, again as 2-D perspective image)|alt=Projection into the <nowiki> </nowiki> y <nowiki> </nowiki> {\displaystyle y} , <nowiki> </nowiki> v <nowiki> </nowiki> {\displaystyle v} , and <nowiki> </nowiki> w <nowiki> </nowiki> {\displaystyle w} <nowiki> </nowiki>dimensions, producing a spiral shape. ( <nowiki> </nowiki> y <nowiki> </nowiki> {\displaystyle y} <nowiki> </nowiki>range extended to ±2π, again as 2-D perspective image). | ||
</gallery> | </gallery> | ||
| Line 257: | Line 269: | ||
The third image shows the graph extended along the real <math>x</math> axis. It shows the graph is a surface of revolution about the <math>x</math> axis of the graph of the real exponential function, producing a horn or funnel shape. | The third image shows the graph extended along the real <math>x</math> axis. It shows the graph is a surface of revolution about the <math>x</math> axis of the graph of the real exponential function, producing a horn or funnel shape. | ||
The fourth image shows the graph extended along the imaginary <math>y</math> axis. It shows that the graph's surface for positive and negative <math>y</math> values doesn't really meet along the negative real <math>v</math> axis, but instead forms a spiral surface about the <math>y</math> axis. Because its <math>y</math> values have been extended to {{math|±2''π''}}, this image also better depicts the | The fourth image shows the graph extended along the imaginary <math>y</math> axis. It shows that the graph's surface for positive and negative <math>y</math> values doesn't really meet along the negative real <math>v</math> axis, but instead forms a spiral surface about the <math>y</math> axis. Because its <math>y</math> values have been extended to {{math|±2''π''}}, this image also better depicts the {{math|2''π''}} periodicity in the imaginary <math>y</math> value. | ||
== | ==Transcendency== | ||
The | The function {{math|''e''{{isup|''z''}}}} is a [[transcendental function]], which means that it is not a [[polynomial root|root]] of a polynomial over the [[field (mathematics)|field]] of the [[rational fraction]]s <math>\C(z);</math> in fact, this is true for any exponential function with a positive real base not equal to 1. | ||
This follows from the stronger statement that if {{math|''a''<sub>1</sub>, ..., ''a''<sub>''n''</sub><nowiki/>}} are distinct complex numbers, then {{math|''e''<sup>''a''<sub>1</sub>''z''</sup>, ..., ''e''<sup>''a''<sub>''n''</sub>''z''</sup><nowiki/>}} are linearly independent over <math>\C(z)</math>. | |||
A much more difficult result is that the base ''e'' of the natural exponential function is a [[transcendental number]], see the [[Lindemann–Weierstrass theorem]]. | |||
=={{anchor|exp|expm1}}Computation== | =={{anchor|exp|expm1}}Computation== | ||
| Line 300: | Line 301: | ||
<math display="block"> e^x = 1 + \cfrac{x}{1 - \cfrac{x}{x + 2 - \cfrac{2x}{x + 3 - \cfrac{3x}{x + 4 - \ddots}}}}</math> | <math display="block"> e^x = 1 + \cfrac{x}{1 - \cfrac{x}{x + 2 - \cfrac{2x}{x + 3 - \cfrac{3x}{x + 4 - \ddots}}}}</math> | ||
The following [[generalized continued fraction]] for {{math|''e''{{isup|''z''}}}} converges more quickly:<ref name="Lorentzen_2008"/> | The following [[generalized continued fraction]] for {{math|''e''{{isup|''z''}}}}, also due to Euler | ||
,<ref>A. N. Khovanski, The applications of continued fractions and their generalization to problems in approximation theory,1963, Noordhoff, Groningen, The Netherlands</ref> | |||
converges more quickly:<ref name="Lorentzen_2008"/> | |||
<math display="block"> e^z = 1 + \cfrac{2z}{2 - z + \cfrac{z^2}{6 + \cfrac{z^2}{10 + \cfrac{z^2}{14 + \ddots}}}}</math> | <math display="block"> e^z = 1 + \cfrac{2z}{2 - z + \cfrac{z^2}{6 + \cfrac{z^2}{10 + \cfrac{z^2}{14 + \ddots}}}}</math> | ||
| Line 311: | Line 314: | ||
<math display="block"> e^3 = 1 + \cfrac{6}{-1 + \cfrac{3^2}{6 + \cfrac{3^2}{10 + \cfrac{3^2}{14 + \ddots }}}} = 13 + \cfrac{54}{7 + \cfrac{9}{14 + \cfrac{9}{18 + \cfrac{9}{22 + \ddots }}}}</math> | <math display="block"> e^3 = 1 + \cfrac{6}{-1 + \cfrac{3^2}{6 + \cfrac{3^2}{10 + \cfrac{3^2}{14 + \ddots }}}} = 13 + \cfrac{54}{7 + \cfrac{9}{14 + \cfrac{9}{18 + \cfrac{9}{22 + \ddots }}}}</math> | ||
==See also== | == Generalizations == | ||
{{ | ===Matrices and Banach algebras=== | ||
The power series definition of the exponential function makes sense for square [[matrix (mathematics)|matrices]] (for which the function is called the [[matrix exponential]]) and more generally in any unital [[Banach algebra]] {{math|''B''}}. In this setting, {{math|1=''e''{{isup|0}} = 1}}, and {{math|''e''{{isup|''x''}}}} is invertible with inverse {{math|''e''{{isup|−''x''}}}} for any {{math|''x''}} in {{math|''B''}}. If {{math|1=''xy'' = ''yx''}}, then {{math|1=''e''{{isup|''x'' + ''y''}} = ''e''{{isup|''x''}}''e''{{isup|''y''}}}}, but this identity can fail for noncommuting {{math|''x''}} and {{math|''y''}}. | |||
Some alternative definitions lead to the same function. For instance, {{math|''e''{{isup|''x''}}}} can be defined as | |||
<math display="block">\lim_{n \to \infty} \left(1 + \frac{x}{n} \right)^n .</math> | |||
Or {{math|''e''{{isup|''x''}}}} can be defined as {{math|''f''<sub>''x''</sub>(1)}}, where {{math|''f''<sub>''x''</sub> : '''R''' → ''B''}} is the solution to the differential equation {{math|1={{sfrac|''df''<sub>''x''</sub>|''dt''}}(''t'') = ''x{{space|hair}}f''<sub>''x''</sub>(''t'')}}, with initial condition {{math|1=''f''<sub>''x''</sub>(0) = 1}}; it follows that {{math|1=''f''<sub>''x''</sub>(''t'') = ''e''{{isup|''tx''}}}} for every {{mvar|t}} in {{math|'''R'''}}. | |||
===Lie algebras=== | |||
Given a [[Lie group]] {{math|''G''}} and its associated [[Lie algebra]] <math>\mathfrak{g}</math>, the [[exponential map (Lie theory)|exponential map]] is a map <math>\mathfrak{g}\to G</math> satisfying similar properties. In fact, since {{math|'''R'''}} is the Lie algebra of the Lie group of all positive real numbers under multiplication, the ordinary exponential function for real arguments is a special case of the Lie algebra situation. Similarly, since the Lie group [[general linear group|{{math|GL(''n'','''R''')}}]] of invertible {{math|''n'' × ''n''}} matrices has as Lie algebra {{math|M(''n'','''R''')}}, the space of all {{math|''n'' × ''n''}} matrices, the exponential function for square matrices is a special case of the Lie algebra exponential map. | |||
The identity <math>\exp(x+y)=\exp(x)\exp(y)</math> can fail for Lie algebra elements {{math|''x''}} and {{math|''y''}} that do not commute; the [[Baker–Campbell–Hausdorff formula]] supplies the necessary correction terms. | |||
== See also == | |||
{{portal|Mathematics}} | |||
{{div col}} | {{div col}} | ||
* [[Carlitz exponential]], a characteristic {{math|''p''}} analogue | * [[Carlitz exponential]], a characteristic {{math|''p''}} analogue | ||
| Line 319: | Line 336: | ||
* [[Gaussian function]] | * [[Gaussian function]] | ||
* [[Half-exponential function]], a compositional square root of an exponential function | * [[Half-exponential function]], a compositional square root of an exponential function | ||
* {{annotated link|Lambert W function#Solving equations}} | * {{annotated link|Lambert W function#Solving equations}} – used for solving exponential equations | ||
* [[List of exponential topics]] | * [[List of exponential topics]] | ||
* [[List of integrals of exponential functions]] | * [[List of integrals of exponential functions]] | ||
| Line 332: | Line 349: | ||
==References== | ==References== | ||
<references> | |||
<!-- <ref name="Rudin_1976">{{Cite book |title=Principles of Mathematical Analysis |author-last=Rudin |author-first=Walter |publisher=[[McGraw-Hill]] |date=1976 |isbn=978-0-07-054235-8 |location=New York |pages=182 |url=https://archive.org/details/PrinciplesOfMathematicalAnalysis}}</ref> --> | <!-- <ref name="Rudin_1976">{{Cite book |title=Principles of Mathematical Analysis |author-last=Rudin |author-first=Walter |publisher=[[McGraw-Hill]] |date=1976 |isbn=978-0-07-054235-8 |location=New York |pages=182 |url=https://archive.org/details/PrinciplesOfMathematicalAnalysis}}</ref> --> | ||
<ref name="Rudin_1987">{{cite book |title=Real and complex analysis |author-last=Rudin |author-first=Walter |date=1987 |publisher=[[McGraw-Hill]] |isbn=978-0-07-054234-1 |edition=3rd |location=New York |page=1 |url=https://archive.org/details/RudinW.RealAndComplexAnalysis3e1987}}</ref> | <ref name="Rudin_1987">{{cite book |title=Real and complex analysis |author-last=Rudin |author-first=Walter |date=1987 |publisher=[[McGraw-Hill]] |isbn=978-0-07-054234-1 |edition=3rd |location=New York |page=1 |url=https://archive.org/details/RudinW.RealAndComplexAnalysis3e1987}}</ref> | ||
| Line 339: | Line 356: | ||
</ref> | </ref> | ||
<ref name="Lorentzen_2008">{{cite book |title=Continued Fractions |chapter=A.2.2 The exponential function. |author-first1=L. |author-last1=Lorentzen|author1-link= Lisa Lorentzen |author-first2=H. |author-last2=Waadeland |series=Atlantis Studies in Mathematics |date=2008 |volume=1 |doi=10.2991/978-94-91216-37-4 |page=268 |isbn=978-94-91216-37-4 |chapter-url=https://link.springer.com/content/pdf/bbm%3A978-94-91216-37-4%2F1}}</ref> | <ref name="Lorentzen_2008">{{cite book |title=Continued Fractions |chapter=A.2.2 The exponential function. |author-first1=L. |author-last1=Lorentzen|author1-link= Lisa Lorentzen |author-first2=H. |author-last2=Waadeland |series=Atlantis Studies in Mathematics |date=2008 |volume=1 |doi=10.2991/978-94-91216-37-4 |page=268 |isbn=978-94-91216-37-4 |chapter-url=https://link.springer.com/content/pdf/bbm%3A978-94-91216-37-4%2F1}}</ref> | ||
<ref name="Apostol_1974">{{Cite book |title=Mathematical Analysis |url=https://archive.org/details/mathematicalanal00apos_530 |url-access=limited |author-last=Apostol |author-first=Tom M. |publisher=[[Addison Wesley]] |date=1974 |isbn=978-0-201-00288-1 |edition=2nd |location=Reading, Mass. |pages=[https://archive.org/details/mathematicalanal00apos_530/page/n32 19]}}</ref> | <ref name="Apostol_1974">{{Cite book |title=Mathematical Analysis |url=https://archive.org/details/mathematicalanal00apos_530 |url-access=limited |author-last=Apostol |author-first=Tom M. |author-link=Tom M. Apostol |publisher=[[Addison Wesley]] |date=1974 |isbn=978-0-201-00288-1 |edition=2nd |location=Reading, Mass. |pages=[https://archive.org/details/mathematicalanal00apos_530/page/n32 19]}}</ref> | ||
<ref name="Beebe_2002">{{cite web |title=Computation of expm1 = exp(x)−1 |author-first=Nelson H. F. |author-last=Beebe |publisher=Department of Mathematics, Center for Scientific Computing, University of Utah |location=Salt Lake City, Utah, USA |date=2002-07-09 |version=1.00 |url=http://www.math.utah.edu/~beebe/reports/expm1.pdf |access-date=2015-11-02}}</ref> | <ref name="Beebe_2002">{{cite web |title=Computation of expm1 = exp(x)−1 |author-first=Nelson H. F. |author-last=Beebe |publisher=Department of Mathematics, Center for Scientific Computing, University of Utah |location=Salt Lake City, Utah, USA |date=2002-07-09 |version=1.00 |url=http://www.math.utah.edu/~beebe/reports/expm1.pdf |access-date=2015-11-02}}</ref> | ||
<ref name="Beebe_2017">{{cite book |author-first=Nelson H. F. |author-last=Beebe |title=The Mathematical-Function Computation Handbook - Programming Using the MathCW Portable Software Library |chapter=Chapter 10.2. Exponential near zero |date=2017-08-22 |location=Salt Lake City, UT, USA |publisher=[[Springer International Publishing AG]] |edition=1 |lccn=2017947446 |isbn=978-3-319-64109-6 |doi=10.1007/978-3-319-64110-2 |pages=273–282 |s2cid=30244721 |quote=Berkeley UNIX 4.3BSD introduced the expm1() function in 1987.}}</ref> | <ref name="Beebe_2017">{{cite book |author-first=Nelson H. F. |author-last=Beebe |title=The Mathematical-Function Computation Handbook - Programming Using the MathCW Portable Software Library |chapter=Chapter 10.2. Exponential near zero |date=2017-08-22 |location=Salt Lake City, UT, USA |publisher=[[Springer International Publishing AG]] |edition=1 |lccn=2017947446 |isbn=978-3-319-64109-6 |doi=10.1007/978-3-319-64110-2 |pages=273–282 |s2cid=30244721 |quote=Berkeley UNIX 4.3BSD introduced the expm1() function in 1987.}}</ref> | ||
| Line 347: | Line 364: | ||
<ref name="Serway-Moses-Moyer_1989">{{cite book |first1=Raymond A. |last1=Serway |first2=Clement J. |last2=Moses |first3=Curt A. |last3=Moyer |date=1989 |isbn=0-03-004844-3 |title=Modern Physics |publisher=[[Harcourt Brace Jovanovich]] |location=Fort Worth |page=384}}</ref> | <ref name="Serway-Moses-Moyer_1989">{{cite book |first1=Raymond A. |last1=Serway |first2=Clement J. |last2=Moses |first3=Curt A. |last3=Moyer |date=1989 |isbn=0-03-004844-3 |title=Modern Physics |publisher=[[Harcourt Brace Jovanovich]] |location=Fort Worth |page=384}}</ref> | ||
<ref name="Simmons_1972">{{cite book |first1=George F. |last1=Simmons |author-link=George F. Simmons |date=1972 |title=Differential Equations with Applications and Historical Notes |publisher=[[McGraw-Hill]] |location=New York |lccn=75173716 |page=15}}</ref> | <ref name="Simmons_1972">{{cite book |first1=George F. |last1=Simmons |author-link=George F. Simmons |date=1972 |title=Differential Equations with Applications and Historical Notes |publisher=[[McGraw-Hill]] |location=New York |lccn=75173716 |page=15}}</ref> | ||
</references> | |||
==External links== | ==External links== | ||