Taylor series of hyperbolic functions


The differentiation rules

dd⁢x⁢cosh⁡x=sinh⁡x,dd⁢x⁢sinh⁡x=cosh⁡x

of the hyperbolic functionsDlmfMathworldPlanetmath imply

d2⁢nd⁢x2⁢ncoshx=coshx,d2⁢n+1d⁢x2⁢n+1coshx=sinhx  (n=0, 1, 2,…).

In the origin  x=0,  all even (http://planetmath.org/Even)-order derivativesPlanetmathPlanetmath of the hyperbolic cosine have the value 1, but the odd (http://planetmath.org/Odd)-order derivatives vanish.  Thus the Taylor seriesMathworldPlanetmath expansion

f⁢(x)=f⁢(0)+f′⁢(0)1!⁢x+f′′⁢(0)2!⁢x2+f′′′⁢(0)3!⁢x3+…

of  f⁢(x):=cosh⁡x  contains only the terms of even degree and writes simply

cosh⁡x= 1+x22!+x44!+…=∑n=0∞x2⁢n(2⁢n)!. (1)

Similarly, one can derive for the hyperbolic sine the expansion

sinh⁡x=x+x33!+x55!+…=∑n=0∞x2⁢n+1(2⁢n+1)!. (2)

Both series converge (http://planetmath.org/AbsoluteConvergence) and the functionsMathworldPlanetmath for all real (and complex) values of x.  Comparing the expansions (1) and (2) with the corresponding ones of the circular functions cosine and sine, one sees easily that

cosh⁡x=cos⁡i⁢x,sinh⁡x=-i⁢sin⁡i⁢x.

As for the Taylor expansion of the third important hyperbolic function tangens hyperbolica (http://planetmath.org/HyperbolicFunctions) tanh, it is obtained via division of the Taylor series (http://planetmath.org/TaylorSeriesViaDivision) (2) and (1); the begin of the quotient series is

tanhx=x-13x3+215x5-17315x7+-…  (|x|<π2). (3)

The coefficients of this power seriesMathworldPlanetmath may be expressed with the Bernoulli numbersDlmfDlmfMathworldPlanetmathPlanetmath.

Title Taylor series of hyperbolic functions
Canonical name TaylorSeriesOfHyperbolicFunctions
Date of creation 2013-03-22 19:07:04
Last modified on 2013-03-22 19:07:04
Owner pahio (2872)
Last modified by pahio (2872)
Numerical id 7
Author pahio (2872)
Entry type Derivation
Classification msc 30B10
Classification msc 26A09
Related topic HyperbolicIdentities
Related topic HigherOrderDerivatives