4.11: Hyperbolic Functions
( \newcommand{\kernel}{\mathrm{null}\,}\)
The hyperbolic functions appear with some frequency in applications, and are quite similar in many respects to the trigonometric functions. This is a bit surprising given our initial definitions.
The hyperbolic cosine is the function
\cosh x ={e^x +e^{-x }\over2},
and the hyperbolic sine is the function
\sinh x ={e^x -e^{-x}\over 2}.
Notice that \cosh is even (that is, \cosh(-x)=\cosh(x)) while \sinh is odd (\sinh(-x)=-\sinh(x)), and \cosh x + \sinh x = e^x. Also, for all x, \cosh x >0, while \sinh x=0 if and only if e^x -e^{-x }=0, which is true precisely when x=0.
The range of \cosh x is [1,\infty).
Let y= \cosh x. We solve for x:
\eqalign{y&={e^x +e^{-x }\over 2}\cr 2y &= e^x + e^{-x }\cr 2ye^x &= e^{2x} + 1\cr 0 &= e^{2x}-2ye^x +1\cr e^{x} &= {2y \pm \sqrt{4y^2 -4}\over 2}\cr e^{x} &= y\pm \sqrt{y^2 -1}\cr}
From the last equation, we see y^2 \geq 1, and since y\geq 0, it follows that y\geq 1.
Now suppose y\geq 1, so y\pm \sqrt{y^2 -1}>0. Then x = \ln(y\pm \sqrt{y^2 -1}) is a real number, and y =\cosh x, so y is in the range of \cosh(x).
\square
The other hyperbolic functions are
\eqalign{\tanh x &= {\sinh x\over\cosh x}\cr \coth x &= {\cosh x\over\sinh x}\cr \text{sech} x &= {1\over\cosh x}\cr \text{csch} x &= {1\over\sinh x}\cr}
The domain of \coth and \text{csch} is x\neq 0 while the domain of the other hyperbolic functions is all real numbers. Graphs are shown in Figure \PageIndex{1}
Certainly the hyperbolic functions do not closely resemble the trigonometric functions graphically. But they do have analogous properties, beginning with the following identity.
For all x in \mathbb{R}, \cosh ^2 x -\sinh ^2 x = 1.
The proof is a straightforward computation:
\cosh ^2 x -\sinh ^2 x = {(e^x +e^{-x} )^2\over 4} -{(e^x -e^{-x} )^2\over 4}= {e^{2x} + 2 + e^{-2x } - e^{2x } + 2 - e^{-2x}\over 4}= {4\over 4} = 1.
\square
This immediately gives two additional identities:
1-\tanh^2 x =\text{sech}^2 x\qquad\hbox{and}\qquad \coth^2 x - 1 =\text{csch}^2 x.
The identity of the theorem also helps to provide a geometric motivation. Recall that the graph of x^2 -y^2 =1 is a hyperbola with asymptotes x=\pm y whose x-intercepts are \pm 1. If (x,y) is a point on the right half of the hyperbola, and if we let x=\cosh t, then y=\pm\sqrt{x^2-1}=\pm\sqrt{\cosh^2x-1}=\pm\sinh t. So for some suitable t, \cosh t and \sinh t are the coordinates of a typical point on the hyperbola. In fact, it turns out that t is twice the area shown in the first graph of Figure \PageIndex{2}. Even this is analogous to trigonometry; \cos t and \sin t are the coordinates of a typical point on the unit circle, and t is twice the area shown in the second graph of Figure \PageIndex{2}.
Given the definitions of the hyperbolic functions, finding their derivatives is straightforward. Here again we see similarities to the trigonometric functions.
{d\over dx}\cosh x=\sinh x and \thmrdef{thm:hyperbolic derivatives} {d\over dx}\sinh x = \cosh x.
{d\over dx}\cosh x= {d\over dx}{e^x +e^{-x}\over 2} = {e^x- e^{-x}\over 2} =\sinh x,
and
{d\over dx}\sinh x = {d\over dx}{e^x -e^{-x}\over 2} = {e^x +e^{-x }\over 2} =\cosh x.
Since \cosh x > 0, \sinh x is increasing and hence injective, so \sinh x has an inverse, \text{arcsinh} x. Also, \sinh x > 0 when x>0, so \cosh x is injective on [0,\infty) and has a (partial) inverse, \text{arccosh} x. The other hyperbolic functions have inverses as well, though \text{arcsech} x is only a partial inverse. We may compute the derivatives of these functions as we have other inverse functions.
{d\over dx}\text{arcsinh} x = {1\over\sqrt{1+x^2}}.
Let y=\text{arcsinh} x, so \sinh y=x. Then
{d\over dx}\sinh y = \cosh(y)\cdot y' = 1,
and so
y' ={1\over\cosh y} ={1\over\sqrt{1 +\sinh^2 y}} = {1\over\sqrt{1+x^2}}.
The other derivatives are left to the exercises.
Contributors
Integrated by Justin Marshall.