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\newtheorem{prop}{Proposition} \newtheorem{cor}{Corollary} \newtheorem*{utheorem}{Theorem} \newtheorem*{ulemma}{Lemma} \newtheorem*{uprop}{Proposition} \newtheorem*{ucor}{Corollary} \theoremstyle{definition} \newtheorem{defn}{Definition} \newtheorem{example}{Example} \newtheorem*{udefn}{Definition} \newtheorem*{uexample}{Example} \theoremstyle{remark} \newtheorem{remark}{Remark} \newtheorem{note}{Note} \newtheorem*{uremark}{Remark} \newtheorem*{unote}{Note} %------------------------------------------------------------------- \begin{document} %------------------------------------------------------------------- \section*{hyperbolic function} [[!redirects hyperbolic functions]] \hypertarget{context}{}\subsubsection*{{Context}}\label{context} \hypertarget{trigonometry}{}\paragraph*{{Trigonometry}}\label{trigonometry} [[!include trigonometry -- contents]] \hypertarget{contents}{}\section*{{Contents}}\label{contents} \noindent\hyperlink{idea}{Idea}\dotfill \pageref*{idea} \linebreak \noindent\hyperlink{definition}{Definition}\dotfill \pageref*{definition} \linebreak \noindent\hyperlink{alternative_presentation}{Alternative presentation}\dotfill \pageref*{alternative_presentation} \linebreak \noindent\hyperlink{related_entries}{Related entries}\dotfill \pageref*{related_entries} \linebreak \hypertarget{idea}{}\subsection*{{Idea}}\label{idea} The hyperbolic functions (or sometimes \emph{hyperbolic trigonometric functions}) are analogues of the usual [[trigonometric functions]], but adapted to the [[hyperbola]] $x^2 - y^2 = 1$ rather than the [[circle]] $x^2 + y^2 = 1$. \hypertarget{definition}{}\subsection*{{Definition}}\label{definition} There are multiple ways of introducing the hyperbolic functions. Probably the most straightforward is to use the following definitions based on the [[exponential function]] $\exp$: \begin{itemize}% \item $\cosh(x) \coloneqq \frac1{2} (\exp(x) + \exp(-x))$ (\emph{hyperbolic cosine}, sometimes pronounced as ``kosh''). This can be interpreted as a function $\mathbb{R} \to \mathbb{R}$, or as a function $\mathbb{C} \to \mathbb{C}$. \item $\sinh(x) \coloneqq \frac1{2} (\exp(x) - \exp(-x))$ (\emph{hyperbolic sine}, sometimes pronounced as ``cinch''). This also can be interpreted as a function $\mathbb{R} \to \mathbb{R}$, or as a function $\mathbb{C} \to \mathbb{C}$. \item The remaining hyperbolic functions are defined by $\tanh \coloneqq \frac{\sinh}{\cosh}$, $\coth = \frac{\cosh}{\sinh}$, $\sech = \frac1{\cosh}$, $\csch = \frac1{\sinh}$. \end{itemize} Note that $(\cosh(t), \sinh(t))$ (as a pair of real-valued functions) lies on the hyperbola $x^2 - y^2 = 1$, and in fact this is a parametrization of the hyperbola, much as $(\cos(t), \sin(t))$ parametrizes the unit circle $x^2 + y^2 = 1$. It is straightforward to establish the following further properties by exploiting properties of the exponential function: \begin{itemize}% \item $\cosh(x + y) = \cosh(x)\cosh(y) + \sinh(x)\sinh(y)$ and $\sinh(x+y) = \sinh(x)\cosh(y) - \cosh(x)\sinh(y)$ (``addition formulas''), \item $(\cosh)' = \sinh$ and $(\sinh)' = \cosh$, \item $\cosh(x + 2\pi i) = \cosh(x)$ and $\sinh(x + 2\pi i) = \sinh(x)$ for all $x \in \mathbb{C}$, \item $\cosh(x) = \sum_{n \geq 0} \frac{x^{2 n}}{(2 n)!}$ and $\sinh(x) = \sum_{n \geq 0} \frac{x^{2 n + 1}}{(2 n + 1)!}$. \end{itemize} \hypertarget{alternative_presentation}{}\subsubsection*{{Alternative presentation}}\label{alternative_presentation} Another avenue is first to introduce the \emph{inverse} hyperbolic functions as [[integrals]] of suitable [[algebraic functions]], e.g., \begin{displaymath} \sinh^{-1}(t) = \int_0^t \; \frac{d x}{y} \end{displaymath} where $y = \sqrt{x^2 + 1}$. Or, what is essentially the same, construct a solution $p(t)$ to the [[differential equation]] \begin{displaymath} (p')^2 = p^2 + 1, \qquad p(0) = 0 \end{displaymath} so that $(p'(t), p(t))$ parametrizes the curve $x^2 - y^2 = 1$; the approach by invoking an integral is in accordance with an elementary method in differential equations that goes by the name ``separation of variables''. This particular approach is similar to the way that [[elliptic functions]] were introduced historically, by studying integrals of algebraic functions \begin{displaymath} \int \; \frac{d x}{y} \end{displaymath} where $y$ is related to $x$ via an algebraic relation such as $y^2 = x^3 + a x + b$. For suitable such relations these give the various so-called \emph{elliptic integrals}; for more on what this has to do with ellipses, see Wikipedia, e.g., \href{http://en.wikipedia.org/wiki/Elliptic_integral#Incomplete_elliptic_integral_of_the_first_kind}{here}. Elliptic functions are then suitable inverses of elliptic integrals, following Jacobi, Abel, and others throughout the nineteenth century (e.g., Weierstrass; see also [[Weierstrass elliptic function]]). \hypertarget{related_entries}{}\subsection*{{Related entries}}\label{related_entries} \begin{itemize}% \item [[trigonometry]] \end{itemize} [[!redirects hyperbolic functions]] [[!redirects hyperbolic trigonometric function]] [[!redirects hyperbolic trigonometric functions]] \end{document}