Calculus The principal motivation for introducing the number , particularly in
calculus, is to perform
differential and
integral calculus with
exponential functions and
logarithms. A general exponential has a derivative, given by a
limit: :\begin{align} \frac{d}{dx}a^x &= \lim_{h\to 0}\frac{a^{x+h} - a^x}{h} = \lim_{h\to 0}\frac{a^x a^h - a^x}{h} \\ &= a^x \cdot \left(\lim_{h\to 0}\frac{a^h - 1}{h}\right). \end{align} The parenthesized limit on the right is independent of the Its value turns out to be the logarithm of to base . Thus, when the value of is set this limit is equal and so one arrives at the following simple identity: :\frac{d}{dx}e^x = e^x. Consequently, the exponential function with base is particularly suited to doing calculus. (as opposed to some other number) as the base of the exponential function makes calculations involving the derivatives much simpler. Another motivation comes from considering the derivative of the base- logarithm (i.e., ), for : :\begin{align} \frac{d}{dx}\log_a x &= \lim_{h\to 0}\frac{\log_a(x + h) - \log_a(x)}{h} \\ &= \lim_{h\to 0}\frac{\log_a(1 + h/x)}{x\cdot h/x} \\ &= \frac{1}{x}\log_a\left(\lim_{u\to 0}(1 + u)^\frac{1}{u}\right) \\ &= \frac{1}{x}\log_a e, \end{align} where the substitution was made. The base- logarithm of is 1, if equals . So symbolically, :\frac{d}{dx}\log_e x = \frac{1}{x}. The logarithm with this special base is called the
natural logarithm, and is usually denoted as ; it behaves well under differentiation since there is no undetermined limit to carry through the calculations. Thus, there are two ways of selecting such special numbers . One way is to set the derivative of the exponential function equal to , and solve for . The other way is to set the derivative of the base logarithm to and solve for . In each case, one arrives at a convenient choice of base for doing calculus. It turns out that these two solutions for are actually
the same: the number . along the The
Taylor series for the exponential function can be deduced from the facts that the exponential function is its own derivative and that it equals 1 when evaluated at 0: e^x = \sum_{n=0}^\infty \frac{x^n}{n!}. Setting x = 1 recovers the definition of as the sum of an infinite series. The natural logarithm function can be defined as the integral from 1 to x of 1/t, and the exponential function can then be defined as the inverse function of the natural logarithm. The number is the value of the exponential function evaluated at x = 1, or equivalently, the number whose natural logarithm is 1. It follows that is the unique positive
real number such that \int_1^e \frac{1}{t} \, dt = 1. Because is the unique function (
up to multiplication by a constant ) that is equal to its own
derivative, \frac{d}{dx}Ke^x = Ke^x, it is therefore its own
antiderivative as well: \int Ke^x\,dx = Ke^x + C . Equivalently, the family of functions y(x) = Ke^x where is any real or complex number, is the full solution to the
differential equation y' = y .
Inequalities The number is the unique real number such that \left(1 + \frac{1}{x}\right)^x for all positive . Also, there is the inequality e^x \ge x + 1 for all real , with equality if and only if . Furthermore, is the unique base of the exponential for which the inequality holds for all . This is a limiting case of
Bernoulli's inequality.
Exponential-like functions of
Steiner's problem asks to find the
global maximum for the function f(x) = x^\frac{1}{x} . This maximum occurs precisely at . (One can check that the derivative of is zero only for this value of .) Similarly, is where the
global minimum occurs for the function f(x) = x^x . The infinite
tetration : x^{x^{x^{\cdot^{\cdot^{\cdot}}}}} or {^\infty}x converges if and only if , shown by a theorem of
Leonhard Euler.
Number theory The real number is
irrational.
Euler proved this by showing that its
simple continued fraction expansion does not terminate. (See also
Fourier's
proof that is irrational.) Furthermore, by the
Lindemann–Weierstrass theorem, is
transcendental, meaning that it is not a solution of any non-zero polynomial equation with rational coefficients. It was the first number to be proved transcendental without having been specifically constructed for this purpose (compare with
Liouville number); the proof was given by
Charles Hermite in 1873. The number is one of only a few transcendental numbers for which the exact
irrationality exponent is known (given by \mu(e)=2). An
unsolved problem thus far is the question of whether or not the numbers and are
algebraically independent. This would be resolved by
Schanuel's conjecture – a currently unproven generalization of the Lindemann–Weierstrass theorem. It is conjectured that is
normal, meaning that when is expressed in any
base the possible digits in that base are uniformly distributed (occur with equal probability in any sequence of given length). In
algebraic geometry, a
period is a number that can be expressed as an integral of an
algebraic function over an algebraic
domain. The constant is a period, but it is conjectured that is not.
Complex numbers The
exponential function may be written as a
Taylor series e^{x} = 1 + {x \over 1!} + {x^{2} \over 2!} + {x^{3} \over 3!} + \cdots = \sum_{n=0}^{\infty} \frac{x^n}{n!}. Because this series is
convergent for every
complex value of , it is commonly used to extend the definition of to the complex numbers. This, with the Taylor series for
and, allows one to derive
Euler's formula: e^{ix} = \cos x + i\sin x , which holds for every complex . Moreover, the identity implies that, in the
principal branch of the logarithm,
Entropy The constant e plays a distinguished role in the theory of
entropy in
probability theory and
ergodic theory. The basic idea is to consider a partition of a
probability space into a finite number of
measurable sets, \xi = (A_1,\cdots, A_k), the entropy of which is the expected information gained regarding the probability distribution by performing a random sample (or "experiment"). The entropy of the partition is H(\xi) = -\sum_{i=1}^k p(A_i)\ln p(A_i). The function f(x) = -x\ln x is thus of fundamental importance, representing the amount of entropy contributed by a particular element of the partition, x=p(A_i). This function is maximized when x=1/e. What this means, concretely, is that the entropy contribution of the particular event A_i is maximized when p(A_i)=1/e; outcomes that are either too likely or too rare contribute less to the total entropy. == Representations ==