Hyperbolic functions

File:Sinh cosh tanh.svg

In mathematics, hyperbolic functions are analogues of the ordinary trigonometric functions, but defined using the hyperbola rather than the circle. Just as the points (cos t, sin t) form a circle with a unit radius, the points (cosh t, sinh t) form the right half of the unit hyperbola. Also, similarly to how the derivatives of sin(t) and cos(t) are cos(t) and –sin(t) respectively, the derivatives of sinh(t) and cosh(t) are cosh(t) and sinh(t) respectively.

Hyperbolic functions are used to express the angle of parallelism in hyperbolic geometry. They are used to express Lorentz boosts as hyperbolic rotations in special relativity. They also occur in the solutions of many linear differential equations (such as the equation defining a catenary), cubic equations, and Laplace's equation in Cartesian coordinates. Laplace's equations are important in many areas of physics, including electromagnetic theory, heat transfer, and fluid dynamics.

The basic hyperbolic functions are:

• hyperbolic sine "sinh" (Template:IPAc-en),
• hyperbolic cosine "cosh" (Template:IPAc-en),

from which are derived:

• hyperbolic tangent "tanh" (Template:IPAc-en),
• hyperbolic cotangent "coth" (Template:IPAc-en),
• hyperbolic secant "sech" (Template:IPAc-en),
• hyperbolic cosecant "csch" or "cosech" (Template:IPAc-en)

corresponding to the derived trigonometric functions.

The inverse hyperbolic functions are:

• inverse hyperbolic sine "arsinh" (also denoted "sinh⁻¹", "asinh" or sometimes "arcsinh")
• inverse hyperbolic cosine "arcosh" (also denoted "cosh⁻¹", "acosh" or sometimes "arccosh")
• inverse hyperbolic tangent "artanh" (also denoted "tanh⁻¹", "atanh" or sometimes "arctanh")
• inverse hyperbolic cotangent "arcoth" (also denoted "coth⁻¹", "acoth" or sometimes "arccoth")
• inverse hyperbolic secant "arsech" (also denoted "sech⁻¹", "asech" or sometimes "arcsech")
• inverse hyperbolic cosecant "arcsch" (also denoted "arcosech", "csch⁻¹", "cosech⁻¹","acsch", "acosech", or sometimes "arccsch" or "arccosech")

File:Hyperbolic functions-2.svg

A ray through the unit hyperbola x² − y² = 1 at the point (cosh a, sinh a), where Template:Mvar is twice the area between the ray, the hyperbola, and the Template:Mvar-axis. For points on the hyperbola below the Template:Mvar-axis, the area is considered negative (see animated version with comparison with the trigonometric (circular) functions).

The hyperbolic functions take an argument called a hyperbolic angle. The magnitude of a hyperbolic angle is the area of its hyperbolic sector to xy = 1. The hyperbolic functions may be defined in terms of the legs of a right triangle covering this sector.

In complex analysis, the hyperbolic functions arise when applying the ordinary sine and cosine functions to an imaginary angle. The hyperbolic sine and the hyperbolic cosine are entire functions. As a result, the other hyperbolic functions are meromorphic in the whole complex plane.

By Lindemann–Weierstrass theorem, the hyperbolic functions have a transcendental value for every non-zero algebraic value of the argument.

History

The first known calculation of a hyperbolic trigonometry problem is attributed to Gerardus Mercator when issuing the Mercator map projection circa 1566. It requires tabulating solutions to a transcendental equation involving hyperbolic functions.

The first to suggest a similarity between the sector of the circle and that of the hyperbola was Isaac Newton in his 1687 Principia Mathematica.

Roger Cotes suggested to modify the trigonometric functions using the imaginary unit $i=\sqrt{-1}$ to obtain an oblate spheroid from a prolate one.

Hyperbolic functions were formally introduced in 1757 by Vincenzo Riccati. Riccati used Sc. and Cc. () to refer to circular functions and Sh. and Ch. () to refer to hyperbolic functions. As early as 1759, Daviet de Foncenex showed the interchangeability of the trigonometric and hyperbolic functions using the imaginary unit and extended de Moivre's formula to hyperbolic functions.

During the 1760s, Johann Heinrich Lambert systematized the use functions and provided exponential expressions in various publications. Lambert credited Riccati for the terminology and names of the functions, but altered the abbreviations to those used today.

Definitions

File:Cartesian hyperbolic rhombus.svg

Right triangles with legs proportional to sinh and cosh

With hyperbolic angle u, the hyperbolic functions sinh and cosh can be defined with the exponential function e^u. In the figure $A=(e^{-u},e^u),B=(e^u,e^{-u}),OA+OB=OC$ .

Exponential definitions

File:Hyperbolic and exponential; sinh.svg

sinh x is half the difference of e^x and e^−x

File:Hyperbolic and exponential; cosh.svg

cosh x is the average of e^x and e^−x

• Hyperbolic sine: the odd part of the exponential function, that is, $$\sinh x=\frac{e^x-e^{-x}}{2}=\frac{e^{2x}-1}{2e^x}.$$
• Hyperbolic cosine: the even part of the exponential function, that is, $$\cosh x=\frac{e^x+e^{-x}}{2}=\frac{e^{2x}+1}{2e^x}.$$

File:Sinh cosh tanh.svg

sinh, cosh and tanh

File:Csch sech coth.svg

csch, sech and coth

• Hyperbolic tangent: $$\tanh x=\frac{\sinh x}{\cosh x}=\frac{e^x-e^{-x}}{e^x+e^{-x}}=\frac{e^{2x}-1}{e^{2x}+1}.$$
• Hyperbolic cotangent: for x ≠ 0, $$\coth x=\frac{\cosh x}{\sinh x}=\frac{e^x+e^{-x}}{e^x-e^{-x}}=\frac{e^{2x}+1}{e^{2x}-1}.$$
• Hyperbolic secant: $$\mathrm{sech}x=\frac{1}{\cosh x}=\frac{2}{e^x+e^{-x}}=\frac{2e^x}{e^{2x}+1}.$$
• Hyperbolic cosecant: for x ≠ 0, $$\mathrm{csch}x=\frac{1}{\sinh x}=\frac{2}{e^x-e^{-x}}=\frac{2e^x}{e^{2x}-1}.$$

Differential equation definitions

The hyperbolic functions may be defined as solutions of differential equations: The hyperbolic sine and cosine are the solution (s, c) of the system $$\begin{array}{rl}{c}^{\prime }(x)& =s(x),\\ s^{\prime }(x)& =c(x),\\ \end{array}$$ with the initial conditions $s(0)=0,c(0)=1.$ The initial conditions make the solution unique; without them any pair of functions $(a{e}^x+b{e}^{-x},a{e}^x-b{e}^{-x})$ would be a solution.

sinh(x) and cosh(x) are also the unique solution of the equation f ″(x) = f (x), such that f (0) = 1, f ′(0) = 0 for the hyperbolic cosine, and f (0) = 0, f ′(0) = 1 for the hyperbolic sine.

Complex trigonometric definitions

Hyperbolic functions may also be deduced from trigonometric functions with complex arguments:

• Hyperbolic sine: $$\sinh x=-i\sin (ix).$$
• Hyperbolic cosine: $$\cosh x=\cos (ix).$$
• Hyperbolic tangent: $$\tanh x=-i\tan (ix).$$
• Hyperbolic cotangent: $$\coth x=i\cot (ix).$$
• Hyperbolic secant: $$\mathrm{sech}x=\sec (ix).$$
• Hyperbolic cosecant:$$\mathrm{csch}x=i\csc (ix).$$

where Template:Mvar is the imaginary unit with i² = −1.

The above definitions are related to the exponential definitions via Euler's formula (See Template:Section link below).

Characterizing properties

Hyperbolic cosine

It can be shown that the area under the curve of the hyperbolic cosine (over a finite interval) is always equal to the arc length corresponding to that interval: $$\text{area}=\underset{a}{\overset{b}{\int }}\cosh xdx=\underset{a}{\overset{b}{\int }}\sqrt{1+{(\frac{d}{dx}\cosh x)}^2}dx=\text{arc length.}$$

Hyperbolic tangent

The hyperbolic tangent is the (unique) solution to the differential equation f ′ = 1 − f ², with f (0) = 0.

Useful relations

The hyperbolic functions satisfy many identities, all of them similar in form to the trigonometric identities. In fact, Osborn's rule (named after George Osborn) states that one can convert any trigonometric identity (up to but not including sinhs or implied sinhs of 4th degree) for $\theta$, $2\theta$, $3\theta$ or $\theta$ and $\phi$ into a hyperbolic identity, by:

1. expanding it completely in terms of integral powers of sines and cosines,
2. changing sine to sinh and cosine to cosh, and
3. switching the sign of every term containing a product of two sinhs.

Odd and even functions: $$\begin{array}{rl}\sinh (-x)& =-\sinh x\\ \cosh (-x)& =\cosh x\\ \tanh (-x)& =-\tanh x\\ \coth (-x)& =-\coth x\\ \mathrm{sech}(-x)& =\mathrm{sech}x\\ \mathrm{csch}(-x)& =-\mathrm{csch}x\end{array}$$

Reciprocals:

$$\begin{array}{rl}\mathrm{arsech}x& =\mathrm{arcosh}\left(\frac{1}{x}\right)\\ \mathrm{arcsch}x& =\mathrm{arsinh}\left(\frac{1}{x}\right)\\ \mathrm{arcoth}x& =\mathrm{artanh}\left(\frac{1}{x}\right)\end{array}$$

Analogous to Euler's formula:

$$\begin{array}{rl}\cosh x+\sinh x& =e^x\\ \cosh x-\sinh x& =e^{-x}\end{array}$$

Analogous to the Pythagorean trigonometric identity:

$$\begin{array}{rl}{\cosh }^{2}x-{\sinh }^{2}x& =1\\ 1-{\tanh }^{2}x& ={\mathrm{sech}}^{2}x\\ {\coth }^{2}x-1& ={\mathrm{csch}}^{2}x\end{array}$$

Sums and differences of arguments

$$\begin{array}{rl}\sinh (x+y)& =\sinh x\cosh y+\cosh x\sinh y\\ \cosh (x+y)& =\cosh x\cosh y+\sinh x\sinh y\\ \tanh (x+y)& =\frac{\tanh x+\tanh y}{1+\tanh x\tanh y}\\ \sinh (x-y)& =\sinh x\cosh y-\cosh x\sinh y\\ \cosh (x-y)& =\cosh x\cosh y-\sinh x\sinh y\\ \tanh (x-y)& =\frac{\tanh x-\tanh y}{1-\tanh x\tanh y}\\ \end{array}$$ particularly $$\begin{array}{rl}\cosh (2x)& ={\sinh }^{2}x+{\cosh }^{2}x=2{\sinh }^{2}x+1=2{\cosh }^{2}x-1\\ \sinh (2x)& =2\sinh x\cosh x\\ \tanh (2x)& =\frac{2\tanh x}{1+{\tanh }^{2}x}\\ \end{array}$$

Addition and subtraction formulas

$$\begin{array}{rl}\sinh x+\sinh y& =2\sinh \left(\frac{x+y}{2}\right)\cosh \left(\frac{x-y}{2}\right)\\ \cosh x+\cosh y& =2\cosh \left(\frac{x+y}{2}\right)\cosh \left(\frac{x-y}{2}\right)\\ \sinh x-\sinh y& =2\cosh \left(\frac{x+y}{2}\right)\sinh \left(\frac{x-y}{2}\right)\\ \cosh x-\cosh y& =2\sinh \left(\frac{x+y}{2}\right)\sinh \left(\frac{x-y}{2}\right)\\ \end{array}$$

Product formulas

$$\begin{array}{rl}\cosh x\cosh y& =\frac{1}{2}(\cosh (x+y)+\cosh (x-y))\\ \sinh x\sinh y& =\frac{1}{2}(\cosh (x+y)-\cosh (x-y))\\ \sinh x\cosh y& =\frac{1}{2}(\sinh (x+y)+\sinh (x-y))\\ \cosh x\sinh y& =\frac{1}{2}(\sinh (x+y)-\sinh (x-y))\\ \end{array}$$

Half argument formulas

$$\begin{array}{rlrl}\sinh \left(\frac{x}{2}\right)& =\frac{\sinh x}{\sqrt{2(\cosh x+1)}}& & =\mathrm{sgn}x\sqrt{\frac{\cosh x-1}{2}}\\ [6px]\cosh \left(\frac{x}{2}\right)& =\sqrt{\frac{\cosh x+1}{2}}\\ [6px]\tanh \left(\frac{x}{2}\right)& =\frac{\sinh x}{\cosh x+1}& & =\mathrm{sgn}x\sqrt{\frac{\cosh x-1}{\cosh x+1}}=\frac{e^x-1}{e^x+1}\end{array}$$

where sgn is the sign function.

If x ≠ 0 then

$$\tanh \left(\frac{x}{2}\right)=\frac{\cosh x-1}{\sinh x}=\coth x-\mathrm{csch}x$$

Tangent half argument formulas

When Template:Tmath, $$\begin{array}{rlrl}& \sinh x=\frac{2t}{1-t^2},& & \cosh x=\frac{1+t^2}{1-t^2},\\ & \tanh x=\frac{2t}{1+t^2},& & \coth x=\frac{1+t^2}{2t},\\ & \mathrm{sech}x=\frac{1-t^2}{1+t^2},& & \mathrm{csch}x=\frac{1-t^2}{2t}.\end{array}$$

Square formulas

$$\begin{array}{rl}{\sinh }^{2}x& =\frac{1}{2}(\cosh 2x-1)\\ {\cosh }^{2}x& =\frac{1}{2}(\cosh 2x+1)\end{array}$$

Inequalities

The following inequality is useful in statistics: $$\cosh (t)\le e^{t^2/2}.$$

It can be proved by comparing the Taylor series of the two functions term by term.

Inverse functions as logarithms

$$\begin{array}{rl}\mathrm{arsinh}(x)& =\ln (x+\sqrt{x^2+1})\\ \mathrm{arcosh}(x)& =\ln (x+\sqrt{x^2-1})& & x\ge 1\\ \mathrm{artanh}(x)& =\frac{1}{2}\ln \left(\frac{1+x}{1-x}\right)& & |x|<1\\ \mathrm{arcoth}(x)& =\frac{1}{2}\ln \left(\frac{x+1}{x-1}\right)& & |x|>1\\ \mathrm{arsech}(x)& =\ln (\frac{1}{x}+\sqrt{\frac{1}{x^2}-1})=\ln \left(\frac{1+\sqrt{1-x^2}}{x}\right)& & 0<x\le 1\\ \mathrm{arcsch}(x)& =\ln (\frac{1}{x}+\sqrt{\frac{1}{x^2}+1})& & x\ne 0\end{array}$$

Derivatives

$$\begin{array}{rl}\frac{d}{dx}\sinh x& =\cosh x\\ \frac{d}{dx}\cosh x& =\sinh x\\ \frac{d}{dx}\tanh x& =1-{\tanh }^{2}x={\mathrm{sech}}^{2}x=\frac{1}{{\cosh }^{2}x}\\ \frac{d}{dx}\coth x& =1-{\coth }^{2}x=-{\mathrm{csch}}^{2}x=-\frac{1}{{\sinh }^{2}x}& & x\ne 0\\ \frac{d}{dx}\mathrm{sech}x& =-\tanh x\mathrm{sech}x\\ \frac{d}{dx}\mathrm{csch}x& =-\coth x\mathrm{csch}x& & x\ne 0\end{array}$$ $$\begin{array}{rl}\frac{d}{dx}\mathrm{arsinh}x& =\frac{1}{\sqrt{x^2+1}}\\ \frac{d}{dx}\mathrm{arcosh}x& =\frac{1}{\sqrt{x^2-1}}& & 1<x\\ \frac{d}{dx}\mathrm{artanh}x& =\frac{1}{1-x^2}& & |x|<1\\ \frac{d}{dx}\mathrm{arcoth}x& =\frac{1}{1-x^2}& & 1<|x|\\ \frac{d}{dx}\mathrm{arsech}x& =-\frac{1}{x\sqrt{1-x^2}}& & 0<x<1\\ \frac{d}{dx}\mathrm{arcsch}x& =-\frac{1}{|x|\sqrt{1+x^2}}& & x\ne 0\end{array}$$

Second derivatives

Each of the functions sinh and cosh is equal to its second derivative, that is: $$\frac{d^2}{d{x}^2}\sinh x=\sinh x$$ $$\frac{d^2}{d{x}^2}\cosh x=\cosh x.$$

All functions with this property are linear combinations of sinh and cosh, in particular the exponential functions $e^x$ and $e^{-x}$.

Standard integrals

$$\begin{array}{rl}\int \sinh (ax)dx& =a^{-1}\cosh (ax)+C\\ \int \cosh (ax)dx& =a^{-1}\sinh (ax)+C\\ \int \tanh (ax)dx& =a^{-1}\ln (\cosh (ax))+C\\ \int \coth (ax)dx& =a^{-1}\ln |\sinh (ax)|+C\\ \int \mathrm{sech}(ax)dx& =a^{-1}\arctan (\sinh (ax))+C\\ \int \mathrm{csch}(ax)dx& =a^{-1}\ln |\tanh \left(\frac{ax}{2}\right)|+C=a^{-1}\ln |\coth \left(ax\right)-\mathrm{csch}\left(ax\right)|+C=-a^{-1}\mathrm{arcoth}(\cosh \left(ax\right))+C\end{array}$$

The following integrals can be proved using hyperbolic substitution: $$\begin{array}{rl}\int \frac{1}{\sqrt{a^2+u^2}}du& =\mathrm{arsinh}\left(\frac{u}{a}\right)+C\\ \int \frac{1}{\sqrt{u^2-a^2}}du& =\mathrm{sgn}u\mathrm{arcosh}\left|\frac{u}{a}\right|+C\\ \int \frac{1}{a^2-u^2}du& =a^{-1}\mathrm{artanh}\left(\frac{u}{a}\right)+C& & u^2<a^2\\ \int \frac{1}{a^2-u^2}du& =a^{-1}\mathrm{arcoth}\left(\frac{u}{a}\right)+C& & u^2>a^2\\ \int \frac{1}{u\sqrt{a^2-u^2}}du& =-a^{-1}\mathrm{arsech}\left|\frac{u}{a}\right|+C\\ \int \frac{1}{u\sqrt{a^2+u^2}}du& =-a^{-1}\mathrm{arcsch}\left|\frac{u}{a}\right|+C\end{array}$$

where C is the constant of integration.

Taylor series expressions

It is possible to express explicitly the Taylor series at zero (or the Laurent series, if the function is not defined at zero) of the above functions.

$$\sinh x=x+\frac{x^3}{3!}+\frac{x^5}{5!}+\frac{x^7}{7!}+\cdots =\sum _{n=0}^{\mathrm{\infty }}\frac{x^{2n+1}}{(2n+1)!}$$ This series is convergent for every complex value of Template:Mvar. Since the function sinh x is odd, only odd exponents for x occur in its Taylor series.

$$\cosh x=1+\frac{x^2}{2!}+\frac{x^4}{4!}+\frac{x^6}{6!}+\cdots =\sum _{n=0}^{\mathrm{\infty }}\frac{x^{2n}}{(2n)!}$$ This series is convergent for every complex value of Template:Mvar. Since the function cosh x is even, only even exponents for Template:Mvar occur in its Taylor series.

The sum of the sinh and cosh series is the infinite series expression of the exponential function.

The following series are followed by a description of a subset of their domain of convergence, where the series is convergent and its sum equals the function. $$\begin{array}{rl}\tanh x& =x-\frac{x^3}{3}+\frac{2x^5}{15}-\frac{17x^7}{315}+\cdots =\sum _{n=1}^{\mathrm{\infty }}\frac{2^{2n}(2^{2n}-1)B_{2n}{x}^{2n-1}}{(2n)!},\left|x\right|<\frac{\pi }{2}\\ \coth x& =x^{-1}+\frac{x}{3}-\frac{x^3}{45}+\frac{2x^5}{945}+\cdots =\sum _{n=0}^{\mathrm{\infty }}\frac{2^{2n}{B}_{2n}{x}^{2n-1}}{(2n)!},0<\left|x\right|<\pi \\ \mathrm{sech}x& =1-\frac{x^2}{2}+\frac{5x^4}{24}-\frac{61x^6}{720}+\cdots =\sum _{n=0}^{\mathrm{\infty }}\frac{E_{2n}{x}^{2n}}{(2n)!},\left|x\right|<\frac{\pi }{2}\\ \mathrm{csch}x& =x^{-1}-\frac{x}{6}+\frac{7x^3}{360}-\frac{31x^5}{15120}+\cdots =\sum _{n=0}^{\mathrm{\infty }}\frac{2(1-2^{2n-1})B_{2n}{x}^{2n-1}}{(2n)!},0<\left|x\right|<\pi \end{array}$$

where:

• $B_n$ is the nth Bernoulli number
• $E_n$ is the nth Euler number

Infinite products and continued fractions

The following expansions are valid in the whole complex plane:

$\sinh x=x\prod _{n=1}^{\mathrm{\infty }}(1+\frac{x^2}{n^2{\pi }^2})=\frac{x}{1-\frac{x^2}{2\cdot 3+x^2-\frac{2\cdot 3x^2}{4\cdot 5+x^2-\frac{4\cdot 5x^2}{6\cdot 7+x^2-\ddots }}}}$

$\cosh x=\prod _{n=1}^{\mathrm{\infty }}(1+\frac{x^2}{(n-1/2{)}^2{\pi }^2})=\frac{1}{1-\frac{x^2}{1\cdot 2+x^2-\frac{1\cdot 2x^2}{3\cdot 4+x^2-\frac{3\cdot 4x^2}{5\cdot 6+x^2-\ddots }}}}$

$\tanh x=\frac{1}{\frac{1}{x}+\frac{1}{\frac{3}{x}+\frac{1}{\frac{5}{x}+\frac{1}{\frac{7}{x}+\ddots }}}}$

Comparison with circular functions

File:Circular and hyperbolic angle.svg

Circle and hyperbola tangent at (1, 1) display geometry of circular functions in terms of circular sector area Template:Mvar and hyperbolic functions depending on hyperbolic sector area Template:Mvar.

The hyperbolic functions represent an expansion of trigonometry beyond the circular functions. Both types depend on an argument, either circular angle or hyperbolic angle.

Since the area of a circular sector with radius Template:Mvar and angle Template:Mvar (in radians) is r²u/2, it will be equal to Template:Mvar when r =

1. REDIRECT Template:Radic

Template:Rcat shell. In the diagram, such a circle is tangent to the hyperbola xy = 1 at (1, 1). The yellow sector depicts an area and angle magnitude. Similarly, the yellow and red regions together depict a hyperbolic sector with area corresponding to hyperbolic angle magnitude.

The legs of the two right triangles with hypotenuse on the ray defining the angles are of length Template:Radic times the circular and hyperbolic functions.

The hyperbolic angle is an invariant measure with respect to the squeeze mapping, just as the circular angle is invariant under rotation.

The Gudermannian function gives a direct relationship between the circular functions and the hyperbolic functions that does not involve complex numbers.

The graph of the function Template:Tmath is the catenary, the curve formed by a uniform flexible chain, hanging freely between two fixed points under uniform gravity.

Relationship to the exponential function

The decomposition of the exponential function in its even and odd parts gives the identities $$e^x=\cosh x+\sinh x,$$ and $$e^{-x}=\cosh x-\sinh x.$$ Combined with Euler's formula $$e^{ix}=\cos x+i\sin x,$$ this gives $$e^{x+iy}=(\cosh x+\sinh x)(\cos y+i\sin y)$$ for the general complex exponential function.

Additionally, $$e^x=\sqrt{\frac{1+\tanh x}{1-\tanh x}}=\frac{1+\tanh \frac{x}{2}}{1-\tanh \frac{x}{2}}$$

Hyperbolic functions for complex numbers

Hyperbolic functions in the complex plane

File:Complex Sinh.jpg	File:Complex Cosh.jpg	File:Complex Tanh.jpg	File:Complex Coth.jpg	File:Complex Sech.jpg	File:Complex Csch.jpg
$\sinh (z)$	$\cosh (z)$	$\tanh (z)$	$\coth (z)$	$\mathrm{sech}(z)$	$\mathrm{csch}(z)$

Since the exponential function can be defined for any complex argument, we can also extend the definitions of the hyperbolic functions to complex arguments. The functions sinh z and cosh z are then holomorphic.

Relationships to ordinary trigonometric functions are given by Euler's formula for complex numbers: $$\begin{array}{rl}{e}^{ix}& =\cos x+i\sin x\\ e^{-ix}& =\cos x-i\sin x\end{array}$$ so: $$\begin{array}{rl}\cosh (ix)& =\frac{1}{2}(e^{ix}+e^{-ix})=\cos x\\ \sinh (ix)& =\frac{1}{2}(e^{ix}-e^{-ix})=i\sin x\\ \tanh (ix)& =i\tan x\\ \cosh (x+iy)& =\cosh (x)\cos (y)+i\sinh (x)\sin (y)\\ \sinh (x+iy)& =\sinh (x)\cos (y)+i\cosh (x)\sin (y)\\ \tanh (x+iy)& =\frac{\tanh (x)+i\tan (y)}{1+i\tanh (x)\tan (y)}\\ \cosh x& =\cos (ix)\\ \sinh x& =-i\sin (ix)\\ \tanh x& =-i\tan (ix)\end{array}$$

Thus, hyperbolic functions are periodic with respect to the imaginary component, with period $2\pi i$ ($\pi i$ for hyperbolic tangent and cotangent).

See also

• e (mathematical constant)
• Equal incircles theorem, based on sinh
• Hyperbolastic functions
• Hyperbolic growth
• Inverse hyperbolic functions
• List of integrals of hyperbolic functions
• Poinsot's spirals
• Sigmoid function
• Trigonometric functions

External links

• Template:Springer
• Hyperbolic functions on PlanetMath
• GonioLab: Visualization of the unit circle, trigonometric and hyperbolic functions (Java Web Start)
• Web-based calculator of hyperbolic functions