Euler's formula

Euler's formula, named after Leonhard Euler, is a mathematical formula in complex analysis that establishes the fundamental relationship between the trigonometric functions and the complex exponential function. Euler's formula states that, for any real number x:

$e^{{ix}}=\cos x+i\sin x$

where e is the base of the natural logarithm, i is the imaginary unit, and cos and sin are the trigonometric functions cosine and sine respectively, with the argument x given in radians. This complex exponential function is sometimes denoted cis x ("cosine plus i sine"). The formula is still valid if x is a complex number, and so some authors refer to the more general complex version as Euler's formula.^[1]

Euler's formula is ubiquitous in mathematics, physics, and engineering. The physicist Richard Feynman called the equation "our jewel" and "the most remarkable formula in mathematics".^[2]

History

Johann Bernoulli noted that^[3]

${\displaystyle {\frac {1}{1+x^{2}}}={\frac {1}{2}}\left({\frac {1}{1-ix}}+{\frac {1}{1+ix}}\right)}$

And since

${\displaystyle \int {\frac {dx}{1+ax}}={\frac {1}{a}}\ln(1+ax)+C}$

the above equation tells us something about complex logarithms. Bernoulli, however, did not evaluate the integral.

Bernoulli's correspondence with Euler (who also knew the above equation) shows that Bernoulli did not fully understand complex logarithms. Euler also suggested that the complex logarithms can have infinitely many values.

Meanwhile, Roger Cotes, in 1714, discovered that

$ix=\ln \left(\cos x+i\sin x\right)$

(ln is the natural logarithm).^[4]

Cotes missed the fact that a complex logarithm can have infinitely many values, differing by multiples of 2iπ, due to the periodicity of the trigonometric functions.

Around 1740 Euler turned his attention to the exponential function instead of logarithms, and obtained the formula used today that is named after him. It was published in 1748, obtained by comparing the series expansions of the exponential and trigonometric expressions.^[4]

None of these mathematicians saw the geometrical interpretation of the formula; the view of complex numbers as points in the complex plane was described some 50 years later by Caspar Wessel.

Applications in complex number theory

Three-dimensional visualization of Euler's formula. See also circular polarization.

This formula can be interpreted as saying that the function e^iφ is a unit complex number, i.e., traces out the unit circle in the complex plane as φ ranges through the real numbers. Here, φ is the angle that a line connecting the origin with a point on the unit circle makes with the positive real axis, measured counter clockwise and in radians.

The original proof is based on the Taylor series expansions of the exponential function e^z (where z is a complex number) and of sin x and cos x for real numbers x (see below). In fact, the same proof shows that Euler's formula is even valid for all complex numbers x.

A point in the complex plane can be represented by a complex number written in cartesian coordinates. Euler's formula provides a means of conversion between cartesian coordinates and polar coordinates. The polar form simplifies the mathematics when used in multiplication or powers of complex numbers. Any complex number z = x + iy, and its complex conjugate, z = x − iy, can be written as

${\displaystyle {\begin{aligned}&z=x+iy=|z|(\cos \varphi +i\sin \varphi )=re^{i\varphi }\\&{\bar {z}}=x-iy=|z|(\cos \varphi -i\sin \varphi )=re^{-i\varphi }\end{aligned}}}$

where

x = Re z, the real part

y = Im z, the imaginary part

r = | z | = √x² + y², the magnitude of z

φ = arg z = atan2(y, x).

φ is the argument of z—i.e., the angle between the x axis and the vector z measured counterclockwise and in radians—which is defined up to addition of 2π. Many texts write φ = tan⁻¹ y/x instead of φ = atan2(y,x), but the first equation needs adjustment when x ≤ 0. This is because, for any real x and y not both zero, the angles of the vectors (x, y) and (−x, −y) differ by π radians, but have the identical value of tan φ = y/x.

Now, taking this derived formula, we can use Euler's formula to define the logarithm of a complex number. To do this, we also use the definition of the logarithm (as the inverse operator of exponentiation) that

${\displaystyle a=e^{\ln a}}$

and that

${\displaystyle e^{a}e^{b}=e^{a+b}}$

both valid for any complex numbers a and b.

Therefore, one can write:

${\displaystyle z=|z|e^{i\varphi }=e^{\ln |z|}e^{i\varphi }=e^{\ln |z|+i\varphi }}$

for any z ≠ 0. Taking the logarithm of both sides shows that:

${\displaystyle \ln z=\ln |z|+i\varphi .}$

and in fact this can be used as the definition for the complex logarithm. The logarithm of a complex number is thus a multi-valued function, because φ is multi-valued.

Finally, the other exponential law

${\displaystyle \left(e^{a}\right)^{k}=e^{ak},}$

which can be seen to hold for all integers k, together with Euler's formula, implies several trigonometric identities as well as de Moivre's formula.

Relationship to trigonometry

Relationship between sine, cosine and exponential function

Euler's formula provides a powerful connection between analysis and trigonometry, and provides an interpretation of the sine and cosine functions as weighted sums of the exponential function:

${\displaystyle {\begin{aligned}\cos x&=\operatorname {Re} \left(e^{ix}\right)={\frac {e^{ix}+e^{-ix}}{2}}\\\sin x&=\operatorname {Im} \left(e^{ix}\right)={\frac {e^{ix}-e^{-ix}}{2i}}\end{aligned}}}$

The two equations above can be derived by adding or subtracting Euler's formulas:

${\displaystyle {\begin{aligned}e^{ix}&=\cos x+i\sin x\\e^{-ix}&=\cos(-x)+i\sin(-x)=\cos x-i\sin x\end{aligned}}}$

and solving for either cosine or sine.

These formulas can even serve as the definition of the trigonometric functions for complex arguments x. For example, letting x = iy, we have:

${\displaystyle {\begin{aligned}\cos(iy)&={\frac {e^{-y}+e^{y}}{2}}=\cosh(y)\\\sin(iy)&={\frac {e^{-y}-e^{y}}{2i}}=-{\frac {e^{y}-e^{-y}}{2i}}=i\sinh(y).\end{aligned}}}$

Complex exponentials can simplify trigonometry, because they are easier to manipulate than their sinusoidal components. One technique is simply to convert sinusoids into equivalent expressions in terms of exponentials. After the manipulations, the simplified result is still real-valued. For example:

${\displaystyle {\begin{aligned}\cos x\cdot \cos y&={\frac {e^{ix}+e^{-ix}}{2}}\cdot {\frac {e^{iy}+e^{-iy}}{2}}\\&={\frac {1}{2}}\cdot {\frac {e^{i(x+y)}+e^{i(x-y)}+e^{i(-x+y)}+e^{i(-x-y)}}{2}}\\&={\frac {1}{2}}{\bigg (}\underbrace {\frac {e^{i(x+y)}+e^{-i(x+y)}}{2}} _{\cos(x+y)}+\underbrace {\frac {e^{i(x-y)}+e^{-i(x-y)}}{2}} _{\cos(x-y)}{\bigg )}\end{aligned}}}$

Another technique is to represent the sinusoids in terms of the real part of a complex expression, and perform the manipulations on the complex expression. For example:

${\displaystyle {\begin{aligned}\cos(nx)&=\operatorname {Re} \left(e^{inx}\right)\\&=\operatorname {Re} \left(e^{i(n-1)x}\cdot e^{ix}\right)\\&=\operatorname {Re} {\Big (}e^{i(n-1)x}\cdot {\big (}\underbrace {e^{ix}+e^{-ix}} _{2\cos x}-e^{-ix}{\big )}{\Big )}\\&=\operatorname {Re} \left(e^{i(n-1)x}\cdot 2\cos x-e^{i(n-2)x}\right)\\&=\cos(n-1)x\cdot 2\cos x-\cos(n-2)x\end{aligned}}}$

This formula is used for recursive generation of cos nx for integer values of n and arbitrary x (in radians).

See also Phasor arithmetic.

Topological interpretation

In the language of topology, Euler's formula states that the imaginary exponential function t ↦ e^it is a (surjective) morphism of topological groups from the real line ℝ to the unit circle ${\mathbb S}$¹. In fact, this exhibits ℝ as a covering space of ${\mathbb S}$¹. Similarly, Euler's identity says that the kernel of this map is τℤ, where τ = 2π. These observations may be combined and summarized in the commutative diagram below:

Other applications

In differential equations, the function e^ix is often used to simplify solutions, even if the final answer is a real function involving sine and cosine. The reason for this is that the exponential function is the eigenfunction of the operation of differentiation.

In electrical engineering, signal processing, and similar fields, signals that vary periodically over time are often described as a combination of sinusoidal functions (see Fourier analysis), and these are more conveniently expressed as the sum of exponential functions with imaginary exponents, using Euler's formula. Also, phasor analysis of circuits can include Euler's formula to represent the impedance of a capacitor or an inductor.

Definitions of complex exponentiation

The exponential function e^x for real values of x may be defined in a few different equivalent ways (see Characterizations of the exponential function). Several of these methods may be directly extended to give definitions of e^z for complex values of z simply by substituting z in place of x and using the complex algebraic operations. In particular we may use either of the two following definitions which are equivalent. From a more advanced perspective, each of these definitions may be interpreted as giving the unique analytic continuation of e^x to the complex plane.

Power series definition

For complex z

${\displaystyle e^{z}=1+{\frac {z}{1!}}+{\frac {z^{2}}{2!}}+{\frac {z^{3}}{3!}}+\cdots =\sum _{n=0}^{\infty }{\frac {z^{n}}{n!}}.}$

Using the ratio test it is possible to show that this power series has an infinite radius of convergence, and so defines e^z for all complex z.

Limit definition

For complex z

${\displaystyle e^{z}=\lim _{n\rightarrow \infty }\left(1+{\frac {z}{n}}\right)^{n}.}$

Proofs

Various proofs of the formula are possible.

Using power series

Here is a proof of Euler's formula using power series expansions as well as basic facts about the powers of i:^[5]

${\displaystyle {\begin{aligned}i^{0}&{}=1,\quad &i^{1}&{}=i,\quad &i^{2}&{}=-1,\quad &i^{3}&{}=-i,\\i^{4}&={}1,\quad &i^{5}&={}i,\quad &i^{6}&{}=-1,\quad &i^{7}&{}=-i\dots \quad {\mbox{etc}}\end{aligned}}}$

Using now the power series definition from above we see that for real values of x

${\displaystyle {\begin{aligned}e^{ix}&{}=1+ix+{\frac {(ix)^{2}}{2!}}+{\frac {(ix)^{3}}{3!}}+{\frac {(ix)^{4}}{4!}}+{\frac {(ix)^{5}}{5!}}+{\frac {(ix)^{6}}{6!}}+{\frac {(ix)^{7}}{7!}}+{\frac {(ix)^{8}}{8!}}+\cdots \\[8pt]&{}=1+ix-{\frac {x^{2}}{2!}}-{\frac {ix^{3}}{3!}}+{\frac {x^{4}}{4!}}+{\frac {ix^{5}}{5!}}-{\frac {x^{6}}{6!}}-{\frac {ix^{7}}{7!}}+{\frac {x^{8}}{8!}}+\cdots \\[8pt]&{}=\left(1-{\frac {x^{2}}{2!}}+{\frac {x^{4}}{4!}}-{\frac {x^{6}}{6!}}+{\frac {x^{8}}{8!}}-\cdots \right)+i\left(x-{\frac {x^{3}}{3!}}+{\frac {x^{5}}{5!}}-{\frac {x^{7}}{7!}}+\cdots \right)\\[8pt]&{}=\cos x+i\sin x.\end{aligned}}}$

In the last step we have simply recognized the Maclaurin series for cos x and sin x. The rearrangement of terms is justified because each series is absolutely convergent.

Using calculus

Another proof^[6] is based on the fact that all complex numbers can be expressed in polar coordinates. Therefore, for some r and θ depending on x,

${\displaystyle e^{ix}=r(\cos \theta +i\sin \theta ).}$

No assumptions are being made about r and θ, they will be determined in the course of the proof. From any of the definitions of the exponential function it can be shown that the derivative of e^ix is ie^ix. Therefore, differentiating both sides gives

${\displaystyle ie^{ix}=(\cos \theta +i\sin \theta ){\frac {dr}{dx}}+r(-\sin \theta +i\cos \theta ){\frac {d\theta }{dx}}.}$

Substituting r(cos θ + i sin θ) for e^ix and equating real and imaginary parts in this formula gives dr/dx = 0 and dθ/dx = 1. Thus, r is a constant and θ is x + C for some constant C. The initial values r(0) = 1 and θ(0) = 0 come from e⁰ⁱ = 1, giving r = 1 and θ = x. This proves the formula

${\displaystyle e^{ix}=1(\cos x+i\sin x)=\cos x+i\sin x.}$

See also

• Complex number
• Euler's identity
• Integration using Euler's formula
• List of topics named after Leonhard Euler

References

1. Moskowitz, Martin A. (2002). A Course in Complex Analysis in One Variable. World Scientific Publishing Co. p. 7. ISBN 981-02-4780-X.
2. Feynman, Richard P. (1977). The Feynman Lectures on Physics, vol. I. Addison-Wesley. p. 22-10. ISBN 0-201-02010-6.
3. Bernoulli, Johann (1702). "Solution d'un problème concernant le calcul intégral, avec quelques abrégés par rapport à ce calcul" [Solution of a problem in integral calculus with some notes relating to this calculation]. Mémoires de l'Académie Royale des Sciences de Paris. 1702: 197–289.
4. John Stillwell (2002). Mathematics and Its History. Springer.
5. Ricardo, Henry J. A Modern Introduction to Differential Equations. p. 428.
6. Strang, Gilbert (1991). Calculus. Wellesley-Cambridge. p. 389. ISBN 0-9614088-2-0. (Second proof on page)

External links

• Hazewinkel, Michiel, ed. (2001), "Euler formulas", Encyclopedia of Mathematics, Springer, ISBN 978-1-55608-010-4
• Complex Exponential Function Module by John H. Mathews
• Elements of Algebra
• Euler's Formula and Euler's Identity : Rationale for Euler's Formula and Euler's Identity, video at Khanacademy.org