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- This article is about Euler's formula in complex analysis. For Euler's formula in algebraic topology and polyhedral combinatorics see Euler characteristic. See also topics named after Euler.

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

- $e^\{ix\}\; =\; cos\; x\; +\; isin\; x\; !$

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, with the argument x given in radians rather than in degrees. 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.

Richard Feynman called Euler's formula "our jewel" and "the most remarkable formula in mathematics".

- $ln(cos\; x\; +\; isin\; x)=ix$

(where "ln" means natural logarithm, i.e. log with base e).

It was Euler who published the equation in its current form in 1748, basing his proof on the infinite series of both sides being equal. Neither of these men saw the geometrical interpretation of the formula: the view of complex numbers as points in the complex plane arose only some 50 years later (see Caspar Wessel). Euler considered it natural to introduce students to complex numbers much earlier than we do today. In his elementary algebra text book, Elements of Algebra, he introduces these numbers almost at once and then uses them in a natural way throughout.

This formula can be interpreted as saying that the function e^{ix} traces out the unit circle in the complex number plane as x ranges through the real numbers. Here, x 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 z.

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 reduces the number of terms from two to one, which simplifies the mathematics when used in multiplication or powers of complex numbers. Any complex number z = x + iy can be written as

- $z\; =\; x\; +\; iy\; =\; |z|\; (cos\; phi\; +\; isin\; phi\; )\; =\; |z|\; e^\{i\; phi\}\; ,$

- $bar\{z\}\; =\; x\; -\; iy\; =\; |z|\; (cos\; phi\; -\; isin\; phi\; )\; =\; |z|\; e^\{-i\; phi\}\; ,$

where

- $x\; =\; mathrm\{Re\}\{z\}\; ,$ the real part

- $y\; =\; mathrm\{Im\}\{z\}\; ,$ the imaginary part

- $|z|\; =\; sqrt\{x^2+y^2\}$ the magnitude of z

- $phi\; =\; ,$ atan2(y, x)

$phi\; ,$ 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.

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

- $a\; =\; e^\{ln\; (a)\},$

and that

- $e^a\; e^b\; =\; e^\{a\; +\; b\},$

both valid for any complex numbers a and b.

Therefore, one can write:

- $z\; =\; |z|\; e^\{i\; phi\}\; =\; e^\{ln\; |z|\}\; e^\{i\; phi\}\; =\; e^\{ln\; |z|\; +\; i\; phi\},$

for any $zne\; 0$. Taking the logarithm of both sides shows that:

- $ln\; z=\; ln\; |z|\; +\; i\; phi.,$

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 $phi\; ,$ is multi-valued.

Finally, the other exponential law

- $(e^a)^k\; =\; e^\{a\; k\},\; ,$

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.

- $cos\; x\; =\; mathrm\{Re\}\{e^\{ix\}\}\; =\{e^\{ix\}\; +\; e^\{-ix\}\; over\; 2\}$

- $sin\; x\; =\; mathrm\{Im\}\{e^\{ix\}\}\; =\{e^\{ix\}\; -\; e^\{-ix\}\; over\; 2i\}$

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

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

- $e^\{-ix\}\; =\; cos(-\; x)\; +\; i\; sin(-\; x)\; =\; cos\; x\; -\; i\; sin\; x\; ;$

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:

- $cos(iy)\; =\; \{e^\{-y\}\; +\; e^\{y\}\; over\; 2\}\; =\; cosh(y)$

- $sin(iy)\; =\; \{e^\{-y\}\; -\; e^\{y\}\; over\; 2i\}\; =\; -isinh(y)$

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:

- $$

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

- $$

This formula is used for recursive generation of a sinusoid at intervals of x radians.

In electrical engineering and other fields, signals that vary periodically over time are often described as a combination of sine and cosine functions (see Fourier analysis), and these are more conveniently expressed as the real part 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.

In general, raising e to a positive integer exponent has a simple interpretation in terms of repeated multiplication of e. Raising e to zero or a negative integer exponent can be understood as repeated division. A rational number exponent can be defined by radicals of e, and an irrational number exponent can be defined by finding rational-number exponents that are arbitrarily close to the irrational-number exponent, in a limit process. However, to define and understand a complex number exponent of e, a different type of generalization is required for the concept of exponentiation.

In fact, several definitions are possible. All of them can be proven to be well-defined and equivalent, although the proofs are not included in this article.

It is well-known that, for any real x, the following series is equal to e^{x}:

- $e^x\; =\; 1\; +\; frac\{x\}\{1!\}\; +\; frac\{x^2\}\{2!\}\; +\; frac\{x^3\}\{3!\}\; +\; cdots\; =\; sum\_\{n=0\}^inftyfrac\{x^n\}\{n!\}~.$

- $e^z\; =\; 1\; +\; frac\{z\}\{1!\}\; +\; frac\{z^2\}\{2!\}\; +\; frac\{z^3\}\{3!\}\; +\; cdots\; ~.$

A simple-to-state, equivalent definition is that e^{z}, for complex z, is the analytic continuation of the function e^{x} for real x. This can be proven to be well-defined; in particular, it yields a single-valued function on the complex plane.

It is well-known that, for any real x, the following limit is equal to e^{x}:

- $e^x\; =\; lim\_\{N\; rightarrow\; infty\}\; left(1+frac\{x\}\{N\}right)^N$

- $e^z\; =\; lim\_\{N\; rightarrow\; infty\}\; left(1+frac\{z\}\{N\}right)^N$

For real x, the function f(x)=e^{x} is well-known to be the unique real function satisfying the differential equation:

- $f\text{'}(x)=f(x),;;;\; f(0)=1$

- $f\text{'}(z)=f(z),;;;\; f(0)=1$

We would expect the function e^{z} to have the following properties:

- $e^\{z\_1\}e^\{z\_2\}\; =\; e^\{z\_1+z\_2\}$
- $e^0\; =\; 1$
- $e^1\; =\; e$
- $e^z$ is continuous

It turns out that this uniquely specifies a function on the complex plane.

Various proofs of this formula are possible. The first proof below starts with the "Taylor series definition" of e^{z}, while the other two use the "Differential equation definition" of e^{z} (see above).

- $begin\{align\}$

and so on. The functions e^{x}, cos x and sin x of the (real) variable x can be expressed using their Taylor expansions around zero:

- $begin\{align\}$

For complex z we define each of these functions by the above series, replacing the real variable x with the complex variable z. This is possible because the radius of convergence of each series is infinite. We then find that

- $begin\{align\}$

The rearrangement of terms is justified because each series is absolutely convergent. Taking z = x to be a real number gives the original identity as Euler discovered it.

- $f(x)\; =\; (cos\; x\; +\; isin\; x)cdot\; e^\{-ix\}.$

The derivative of ƒ(x), according to the product rule, is:

- $begin\{align\}$

Therefore, ƒ(x) must be a constant function in x. Because ƒ(0) is known, the constant that ƒ(x) equals for all real x is also known. Thus,

- $(cos\; x\; +\; isin\; x)cdot\; e^\{-ix\}\; =\; f(x)\; =\; f(0)\; =\; (cos\; 0\; +\; isin\; 0)cdot\; e^0\; =\; 1\; ,.$

Multiplying both sides by e^{ix} and using

- $e^\{-ix\}\; cdot\; e^\{ix\}\; =\; e^\{-ix\; ,\; +\; ,\; ix\}\; =\; e^0\; =\; 1\; ,,$

it follows that

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

- $g(x)\; stackrel\{mathrm\{def\}\}\{=\}\; e^\{ix\}\; .$

Considering that i is constant, the first and second derivatives of g(x) are

- $g\text{'}(x)\; =\; i\; e^\{ix\}$

- $g(x)\; =\; i^2\; e^\{ix\}\; =\; -e^\{ix\}$

because i^{ 2} = −1 by definition. From this the following 2^{nd}-order linear ordinary differential equation is constructed:

- $g(x)\; =\; -g(x)$

- $g\text{'}\text{'}(x)\; +\; g(x)\; =\; 0.$

Being a 2^{nd}-order differential equation, there are two linearly independent solutions that satisfy it:

- $g\_1(x)\; =\; cos\; x$

- $g\_2(x)\; =\; sin\; x.$

Both cos and sin are real functions in which the 2^{nd} derivative is identical to the negative of that function. Any linear combination of solutions to a homogeneous differential equation is also a solution. Then, in general, the solution to the differential equation is

$g(x),$ $=\; A\; g\_1(x)\; +\; B\; g\_2(x)$ $=\; A\; cos\; x\; +\; B\; sin\; x$ for any constants A and B. But not all values of these two constants satisfy the known initial conditions for g(x):

- $g(0)\; =\; e^\{i0\}\; =\; 1$

- $g\text{'}(0)\; =\; i\; e^\{i0\}\; =\; i$.

However these same initial conditions (applied to the general solution) are

- $g(0)\; =\; A\; cos\; 0\; +\; B\; sin\; 0\; =\; A$

- $g\text{'}(0)\; =\; -A\; sin\; 0\; +\; B\; cos\; 0\; =\; B$

resulting in

- $g(0)\; =\; A\; =\; 1$

- $g\text{'}(0)\; =\; B\; =\; i$

and, finally,

- $g(x)\; stackrel\{mathrm\{def\}\}\{=\}\; e^\{ix\}\; =\; cos\; x\; +\; i\; sin\; x.$

## See also

- Leonhard Euler
- Euler's identity
- Complex number
- de Moivre's formula
- Exponentiation
- Exponential function

## References

## External links

- Proof of Euler's Formula by Julius O. Smith III
- Euler's Formula and Fermat's Last Theorem
- Complex Exponential Function Module by John H. Mathews
- Elements of Algebra
- Visual Representation of Euler's Formula

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This article is licensed under the GNU Free Documentation License.

Last updated on Thursday October 09, 2008 at 16:02:11 PDT (GMT -0700)

View this article at Wikipedia.org - Edit this article at Wikipedia.org - Donate to the Wikimedia Foundation

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