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Mathematics · Ch 13 — Hyperbolic Functions

Identities, Addition Formulas and Logarithmic Forms

13.4

Identities, Addition Formulas and Logarithmic Forms

Fundamental identities. From the definitions, cosh⁡2x−sinh⁡2x=(ex+e−x2)2−(ex−e−x2)2=(e2x+2+e−2x)−(e2x−2+e−2x)4=44=1\cosh^2 x - \sinh^2 x = \left(\frac{e^x+e^{-x}}{2}\right)^2 - \left(\frac{e^x-e^{-x}}{2}\right)^2 = \frac{(e^{2x}+2+e^{-2x}) - (e^{2x}-2+e^{-2x})}{4} = \frac{4}{4} = 1 for every real xx — the hyperbolic analogue of cos⁡2θ+sin⁡2θ=1\cos^2\theta+\sin^2\theta=1, but with a minus sign, which is exactly why these are called hyperbolic functions: the point (cosh⁡x,sinh⁡x)(\cosh x, \sinh x) traces the right branch of the hyperbola u2−v2=1u^2 - v^2 = 1, just as (cos⁡θ,sin⁡θ)(\cos\theta,\sin\theta) traces the unit circle. Dividing through by cosh⁡2x\cosh^2 x gives 1−tanh⁡2x=sech⁡2x1 - \tanh^2 x = \operatorname{sech}^2 x, and dividing by sinh⁡2x\sinh^2 x gives coth⁡2x−1=csch⁡2x\coth^2 x - 1 = \operatorname{csch}^2 x.

Addition formulas (Theorem 9.3.1). For all real x,yx,y:

sinh⁡(x±y)=sinh⁡xcosh⁡y±cosh⁡xsinh⁡y,cosh⁡(x±y)=cosh⁡xcosh⁡y±sinh⁡xsinh⁡y,\sinh(x\pm y) = \sinh x\cosh y \pm \cosh x\sinh y, \qquad \cosh(x\pm y) = \cosh x\cosh y \pm \sinh x\sinh y,

tanh⁡(x±y)=tanh⁡x±tanh⁡y1±tanh⁡xtanh⁡y.\tanh(x\pm y) = \frac{\tanh x \pm \tanh y}{1 \pm \tanh x\tanh y}.

Proof (for sinh⁡(x+y)\sinh(x+y)). Writing everything in terms of exe^x: sinh⁡xcosh⁡y+cosh⁡xsinh⁡y=(ex−e−x)(ey+e−y)+(ex+e−x)(ey−e−y)4\sinh x\cosh y + \cosh x\sinh y = \frac{(e^x-e^{-x})(e^y+e^{-y}) + (e^x+e^{-x})(e^y-e^{-y})}{4}. Expanding both products and adding, the cross-terms ex−ye^{x-y} and −ex−y-e^{x-y} (and similarly ey−xe^{y-x}) cancel, leaving 2ex+y−2e−(x+y)4=ex+y−e−(x+y)2=sinh⁡(x+y)\frac{2e^{x+y} - 2e^{-(x+y)}}{4} = \frac{e^{x+y}-e^{-(x+y)}}{2} = \sinh(x+y). The cosh⁡\cosh and tanh⁡\tanh addition formulas, and the minus-sign versions, follow by the same expansion or by substituting y→−yy \to -y and using the parities from §9.1.

Double-angle corollaries. Setting y=xy=x: sinh⁡2x=2sinh⁡xcosh⁡x\sinh 2x = 2\sinh x\cosh x, and cosh⁡2x=cosh⁡2x+sinh⁡2x=2cosh⁡2x−1=1+2sinh⁡2x\cosh 2x = \cosh^2 x+\sinh^2x = 2\cosh^2x-1 = 1+2\sinh^2x (the last two forms follow by substituting cosh⁡2x−sinh⁡2x=1\cosh^2x-\sinh^2x=1).

Logarithmic forms of the inverse functions. These theorems convert an inverse hyperbolic function into an explicit logarithm, which is what makes numerical evaluation possible.

Theorem: sinh⁡−1x=log⁡(x+x2+1)\sinh^{-1}x=\log\left(x+\sqrt{x^2+1}\right) for all real xx. Proof: let y=sinh⁡−1xy=\sinh^{-1}x, so x=sinh⁡y=ey−e−y2x=\sinh y=\frac{e^y-e^{-y}}{2}, i.e. e2y−2xey−1=0e^{2y}-2xe^y-1=0, a quadratic in eye^y. Solving, ey=2x±4x2+42=x±x2+1e^y=\frac{2x\pm\sqrt{4x^2+4}}{2}=x\pm\sqrt{x^2+1}; since ey>0e^y>0 and x2+1>∣x∣\sqrt{x^2+1}>|x|, only the ++ sign is admissible, giving ey=x+x2+1e^y=x+\sqrt{x^2+1} and hence y=log⁡(x+x2+1)y=\log\left(x+\sqrt{x^2+1}\right). …