Collective name of 6 mathematical functions
"Hyperbolic curve" redirects here. For the geometric curve, see
Hyperbola .
Inmathematics ,hyperbolic functions are analogues of the ordinarytrigonometric functions ,but defined using thehyperbola rather than thecircle .Just as the points(cost ,sint ) form acircle with a unit radius ,the points(cosht ,sinht ) form the right half of theunit hyperbola .Also, similarly to how the derivatives ofsin(t ) andcos(t ) arecos(t ) and–sin(t ) respectively, the derivatives ofsinh(t ) andcosh(t ) arecosh(t ) and+sinh(t ) respectively.
Hyperbolic functions occur in the calculations of angles and distances inhyperbolic geometry .They also occur in the solutions of many lineardifferential equations (such as the equation defining acatenary ),cubic equations ,andLaplace's equation inCartesian coordinates .Laplace's equations are important in many areas ofphysics ,includingelectromagnetic theory ,heat transfer ,fluid dynamics ,andspecial relativity .
The basic hyperbolic functions are:[ 1]
hyperbolic sine "sinh "(),[ 2]
hyperbolic cosine "cosh "(),[ 3]
from which are derived:[ 4]
hyperbolic tangent "tanh "(),[ 5]
hyperbolic cotangent "coth "(),[ 6] [ 7]
hyperbolic secant "sech "(),[ 8]
hyperbolic cosecant "csch "or"cosech "([ 3] )
corresponding to the derived trigonometric functions.
Theinverse hyperbolic functions are:
area hyperbolic sine "arsinh "(also denoted"sinh−1 ","asinh "or sometimes"arcsinh ")[ 9] [ 10] [ 11]
area hyperbolic cosine "arcosh "(also denoted"cosh−1 ","acosh "or sometimes"arccosh ")
area hyperbolic tangent "artanh "(also denoted"tanh−1 ","atanh "or sometimes"arctanh ")
area hyperbolic cotangent "arcoth "(also denoted"coth−1 ","acoth "or sometimes"arccoth ")
area hyperbolic secant "arsech "(also denoted"sech−1 ","asech "or sometimes"arcsech ")
area hyperbolic cosecant "arcsch "(also denoted"arcosech ","csch−1 ","cosech−1 ","acsch ","acosech ",or sometimes"arccsch "or"arccosech ")
Aray through theunit hyperbola x 2 −y 2 = 1 at the point(cosha ,sinha ) ,wherea is twice the area between the ray, the hyperbola, and thex -axis. For points on the hyperbola below thex -axis, the area is considered negative (seeanimated version with comparison with the trigonometric (circular) functions).
The hyperbolic functions take areal argument called ahyperbolic angle .The size of a hyperbolic angle is twice the area of itshyperbolic sector .The hyperbolic functions may be defined in terms of thelegs of a right triangle covering this sector.
Incomplex analysis ,the hyperbolic functions arise when applying the ordinary sine and cosine functions to an imaginary angle. The hyperbolic sine and the hyperbolic cosine areentire functions .As a result, the other hyperbolic functions aremeromorphic in the whole complex plane.
ByLindemann–Weierstrass theorem ,the hyperbolic functions have atranscendental value for every non-zeroalgebraic value of the argument.[ 12]
Hyperbolic functions were introduced in the 1760s independently byVincenzo Riccati andJohann Heinrich Lambert .[ 13] Riccati usedSc. andCc. (sinus/cosinus circulare ) to refer to circular functions andSh. andCh. (sinus/cosinus hyperbolico ) to refer to hyperbolic functions. Lambert adopted the names, but altered the abbreviations to those used today.[ 14] The abbreviationssh ,ch ,th ,cth are also currently used, depending on personal preference.
sinh ,cosh andtanh
csch ,sech andcoth
There are various equivalent ways to define the hyperbolic functions.
Exponential definitions [ edit ]
sinhx is half thedifference ofex ande −x
coshx is theaverage ofex ande −x
In terms of theexponential function :[ 1] [ 4]
Hyperbolic sine: theodd part of the exponential function, that is,
sinh
x
=
e
x
−
e
−
x
2
=
e
2
x
−
1
2
e
x
=
1
−
e
−
2
x
2
e
−
x
.
{\displaystyle \sinh x={\frac {e^{x}-e^{-x}}{2}}={\frac {e^{2x}-1}{2e^{x}}}={\frac {1-e^{-2x}}{2e^{-x}}}.}
Hyperbolic cosine: theeven part of the exponential function, that is,
cosh
x
=
e
x
+
e
−
x
2
=
e
2
x
+
1
2
e
x
=
1
+
e
−
2
x
2
e
−
x
.
{\displaystyle \cosh x={\frac {e^{x}+e^{-x}}{2}}={\frac {e^{2x}+1}{2e^{x}}}={\frac {1+e^{-2x}}{2e^{-x}}}.}
Hyperbolic tangent:
tanh
x
=
sinh
x
cosh
x
=
e
x
−
e
−
x
e
x
+
e
−
x
=
e
2
x
−
1
e
2
x
+
1
.
{\displaystyle \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: forx ≠ 0 ,
coth
x
=
cosh
x
sinh
x
=
e
x
+
e
−
x
e
x
−
e
−
x
=
e
2
x
+
1
e
2
x
−
1
.
{\displaystyle \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:
sech
x
=
1
cosh
x
=
2
e
x
+
e
−
x
=
2
e
x
e
2
x
+
1
.
{\displaystyle \operatorname {sech} x={\frac {1}{\cosh x}}={\frac {2}{e^{x}+e^{-x}}}={\frac {2e^{x}}{e^{2x}+1}}.}
Hyperbolic cosecant: forx ≠ 0 ,
csch
x
=
1
sinh
x
=
2
e
x
−
e
−
x
=
2
e
x
e
2
x
−
1
.
{\displaystyle \operatorname {csch} x={\frac {1}{\sinh x}}={\frac {2}{e^{x}-e^{-x}}}={\frac {2e^{x}}{e^{2x}-1}}.}
Differential equation definitions [ edit ]
The hyperbolic functions may be defined as solutions ofdifferential equations :The hyperbolic sine and cosine are the solution(s ,c ) of the system
c
′
(
x
)
=
s
(
x
)
,
s
′
(
x
)
=
c
(
x
)
,
{\displaystyle {\begin{aligned}c'(x)&=s(x),\\s'(x)&=c(x),\\\end{aligned}}}
with the initial conditions
s
(
0
)
=
0
,
c
(
0
)
=
1.
{\displaystyle 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
)
{\displaystyle (ae^{x}+be^{-x},ae^{x}-be^{-x})}
would be a solution.
sinh(x ) andcosh(x ) are also the unique solution of the equationf ″(x ) =f (x ) ,
such thatf (0) = 1 ,f ′(0) = 0 for the hyperbolic cosine, andf (0) = 0 ,f ′(0) = 1 for the hyperbolic sine.
Complex trigonometric definitions [ edit ]
Hyperbolic functions may also be deduced fromtrigonometric functions withcomplex arguments:
Hyperbolic sine:[ 1]
sinh
x
=
−
i
sin
(
i
x
)
.
{\displaystyle \sinh x=-i\sin(ix).}
Hyperbolic cosine:[ 1]
cosh
x
=
cos
(
i
x
)
.
{\displaystyle \cosh x=\cos(ix).}
Hyperbolic tangent:
tanh
x
=
−
i
tan
(
i
x
)
.
{\displaystyle \tanh x=-i\tan(ix).}
Hyperbolic cotangent:
coth
x
=
i
cot
(
i
x
)
.
{\displaystyle \coth x=i\cot(ix).}
Hyperbolic secant:
sech
x
=
sec
(
i
x
)
.
{\displaystyle \operatorname {sech} x=\sec(ix).}
Hyperbolic cosecant:
csch
x
=
i
csc
(
i
x
)
.
{\displaystyle \operatorname {csch} x=i\csc(ix).}
wherei is theimaginary unit withi 2 = −1 .
The above definitions are related to the exponential definitions viaEuler's formula (See§ Hyperbolic functions for complex numbers below).
Characterizing properties [ edit ]
It can be shown that thearea under the curve of the hyperbolic cosine (over a finite interval) is always equal to thearc length corresponding to that interval:[ 15]
area
=
∫
a
b
cosh
x
d
x
=
∫
a
b
1
+
(
d
d
x
cosh
x
)
2
d
x
=
arc length.
{\displaystyle {\text{area}}=\int _{a}^{b}\cosh x\,dx=\int _{a}^{b}{\sqrt {1+\left({\frac {d}{dx}}\cosh x\right)^{2}}}\,dx={\text{arc length.}}}
The hyperbolic tangent is the (unique) solution to thedifferential equation f ′ = 1 −f 2 ,withf (0) = 0 .[ 16] [ 17]
The hyperbolic functions satisfy many identities, all of them similar in form to thetrigonometric identities .In fact,Osborn's rule [ 18] states that one can convert any trigonometric identity (up to but not including sinhs or implied sinhs of 4th degree) for
θ
{\displaystyle \theta }
,
2
θ
{\displaystyle 2\theta }
,
3
θ
{\displaystyle 3\theta }
or
θ
{\displaystyle \theta }
and
φ
{\displaystyle \varphi }
into a hyperbolic identity, by expanding it completely in terms of integral powers of sines and cosines, changing sine to sinh and cosine to cosh, and switching the sign of every term containing a product of two sinhs.
Odd and even functions:
sinh
(
−
x
)
=
−
sinh
x
cosh
(
−
x
)
=
cosh
x
{\displaystyle {\begin{aligned}\sinh(-x)&=-\sinh x\\\cosh(-x)&=\cosh x\end{aligned}}}
Hence:
tanh
(
−
x
)
=
−
tanh
x
coth
(
−
x
)
=
−
coth
x
sech
(
−
x
)
=
sech
x
csch
(
−
x
)
=
−
csch
x
{\displaystyle {\begin{aligned}\tanh(-x)&=-\tanh x\\\coth(-x)&=-\coth x\\\operatorname {sech} (-x)&=\operatorname {sech} x\\\operatorname {csch} (-x)&=-\operatorname {csch} x\end{aligned}}}
Thus,coshx andsechx areeven functions ;the others areodd functions .
arsech
x
=
arcosh
(
1
x
)
arcsch
x
=
arsinh
(
1
x
)
arcoth
x
=
artanh
(
1
x
)
{\displaystyle {\begin{aligned}\operatorname {arsech} x&=\operatorname {arcosh} \left({\frac {1}{x}}\right)\\\operatorname {arcsch} x&=\operatorname {arsinh} \left({\frac {1}{x}}\right)\\\operatorname {arcoth} x&=\operatorname {artanh} \left({\frac {1}{x}}\right)\end{aligned}}}
Hyperbolic sine and cosine satisfy:
cosh
x
+
sinh
x
=
e
x
cosh
x
−
sinh
x
=
e
−
x
cosh
2
x
−
sinh
2
x
=
1
{\displaystyle {\begin{aligned}\cosh x+\sinh x&=e^{x}\\\cosh x-\sinh x&=e^{-x}\\\cosh ^{2}x-\sinh ^{2}x&=1\end{aligned}}}
the last of which is similar to thePythagorean trigonometric identity .
One also has
sech
2
x
=
1
−
tanh
2
x
csch
2
x
=
coth
2
x
−
1
{\displaystyle {\begin{aligned}\operatorname {sech} ^{2}x&=1-\tanh ^{2}x\\\operatorname {csch} ^{2}x&=\coth ^{2}x-1\end{aligned}}}
for the other functions.
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
)
=
tanh
x
+
tanh
y
1
+
tanh
x
tanh
y
{\displaystyle {\begin{aligned}\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{aligned}}}
particularly
cosh
(
2
x
)
=
sinh
2
x
+
cosh
2
x
=
2
sinh
2
x
+
1
=
2
cosh
2
x
−
1
sinh
(
2
x
)
=
2
sinh
x
cosh
x
tanh
(
2
x
)
=
2
tanh
x
1
+
tanh
2
x
{\displaystyle {\begin{aligned}\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{aligned}}}
Also:
sinh
x
+
sinh
y
=
2
sinh
(
x
+
y
2
)
cosh
(
x
−
y
2
)
cosh
x
+
cosh
y
=
2
cosh
(
x
+
y
2
)
cosh
(
x
−
y
2
)
{\displaystyle {\begin{aligned}\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)\\\end{aligned}}}
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
)
=
tanh
x
−
tanh
y
1
−
tanh
x
tanh
y
{\displaystyle {\begin{aligned}\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{aligned}}}
Also:[ 19]
sinh
x
−
sinh
y
=
2
cosh
(
x
+
y
2
)
sinh
(
x
−
y
2
)
cosh
x
−
cosh
y
=
2
sinh
(
x
+
y
2
)
sinh
(
x
−
y
2
)
{\displaystyle {\begin{aligned}\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{aligned}}}
sinh
(
x
2
)
=
sinh
x
2
(
cosh
x
+
1
)
=
sgn
x
cosh
x
−
1
2
cosh
(
x
2
)
=
cosh
x
+
1
2
tanh
(
x
2
)
=
sinh
x
cosh
x
+
1
=
sgn
x
cosh
x
−
1
cosh
x
+
1
=
e
x
−
1
e
x
+
1
{\displaystyle {\begin{aligned}\sinh \left({\frac {x}{2}}\right)&={\frac {\sinh x}{\sqrt {2(\cosh x+1)}}}&&=\operatorname {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}}&&=\operatorname {sgn} x\,{\sqrt {\frac {\cosh x-1}{\cosh x+1}}}={\frac {e^{x}-1}{e^{x}+1}}\end{aligned}}}
wheresgn is thesign function .
Ifx ≠ 0 ,then[ 20]
tanh
(
x
2
)
=
cosh
x
−
1
sinh
x
=
coth
x
−
csch
x
{\displaystyle \tanh \left({\frac {x}{2}}\right)={\frac {\cosh x-1}{\sinh x}}=\coth x-\operatorname {csch} x}
sinh
2
x
=
1
2
(
cosh
2
x
−
1
)
cosh
2
x
=
1
2
(
cosh
2
x
+
1
)
{\displaystyle {\begin{aligned}\sinh ^{2}x&={\tfrac {1}{2}}(\cosh 2x-1)\\\cosh ^{2}x&={\tfrac {1}{2}}(\cosh 2x+1)\end{aligned}}}
The following inequality is useful in statistics:[ 21]
cosh
(
t
)
≤
e
t
2
/
2
.
{\displaystyle \operatorname {cosh} (t)\leq e^{t^{2}/2}.}
It can be proved by comparing the Taylor series of the two functions term by term.
Inverse functions as logarithms [ edit ]
arsinh
(
x
)
=
ln
(
x
+
x
2
+
1
)
arcosh
(
x
)
=
ln
(
x
+
x
2
−
1
)
x
≥
1
artanh
(
x
)
=
1
2
ln
(
1
+
x
1
−
x
)
|
x
|
<
1
arcoth
(
x
)
=
1
2
ln
(
x
+
1
x
−
1
)
|
x
|
>
1
arsech
(
x
)
=
ln
(
1
x
+
1
x
2
−
1
)
=
ln
(
1
+
1
−
x
2
x
)
0
<
x
≤
1
arcsch
(
x
)
=
ln
(
1
x
+
1
x
2
+
1
)
x
≠
0
{\displaystyle {\begin{aligned}\operatorname {arsinh} (x)&=\ln \left(x+{\sqrt {x^{2}+1}}\right)\\\operatorname {arcosh} (x)&=\ln \left(x+{\sqrt {x^{2}-1}}\right)&&x\geq 1\\\operatorname {artanh} (x)&={\frac {1}{2}}\ln \left({\frac {1+x}{1-x}}\right)&&|x|<1\\\operatorname {arcoth} (x)&={\frac {1}{2}}\ln \left({\frac {x+1}{x-1}}\right)&&|x|>1\\\operatorname {arsech} (x)&=\ln \left({\frac {1}{x}}+{\sqrt {{\frac {1}{x^{2}}}-1}}\right)=\ln \left({\frac {1+{\sqrt {1-x^{2}}}}{x}}\right)&&0<x\leq 1\\\operatorname {arcsch} (x)&=\ln \left({\frac {1}{x}}+{\sqrt {{\frac {1}{x^{2}}}+1}}\right)&&x\neq 0\end{aligned}}}
d
d
x
sinh
x
=
cosh
x
d
d
x
cosh
x
=
sinh
x
d
d
x
tanh
x
=
1
−
tanh
2
x
=
sech
2
x
=
1
cosh
2
x
d
d
x
coth
x
=
1
−
coth
2
x
=
−
csch
2
x
=
−
1
sinh
2
x
x
≠
0
d
d
x
sech
x
=
−
tanh
x
sech
x
d
d
x
csch
x
=
−
coth
x
csch
x
x
≠
0
{\displaystyle {\begin{aligned}{\frac {d}{dx}}\sinh x&=\cosh x\\{\frac {d}{dx}}\cosh x&=\sinh x\\{\frac {d}{dx}}\tanh x&=1-\tanh ^{2}x=\operatorname {sech} ^{2}x={\frac {1}{\cosh ^{2}x}}\\{\frac {d}{dx}}\coth x&=1-\coth ^{2}x=-\operatorname {csch} ^{2}x=-{\frac {1}{\sinh ^{2}x}}&&x\neq 0\\{\frac {d}{dx}}\operatorname {sech} x&=-\tanh x\operatorname {sech} x\\{\frac {d}{dx}}\operatorname {csch} x&=-\coth x\operatorname {csch} x&&x\neq 0\end{aligned}}}
d
d
x
arsinh
x
=
1
x
2
+
1
d
d
x
arcosh
x
=
1
x
2
−
1
1
<
x
d
d
x
artanh
x
=
1
1
−
x
2
|
x
|
<
1
d
d
x
arcoth
x
=
1
1
−
x
2
1
<
|
x
|
d
d
x
arsech
x
=
−
1
x
1
−
x
2
0
<
x
<
1
d
d
x
arcsch
x
=
−
1
|
x
|
1
+
x
2
x
≠
0
{\displaystyle {\begin{aligned}{\frac {d}{dx}}\operatorname {arsinh} x&={\frac {1}{\sqrt {x^{2}+1}}}\\{\frac {d}{dx}}\operatorname {arcosh} x&={\frac {1}{\sqrt {x^{2}-1}}}&&1<x\\{\frac {d}{dx}}\operatorname {artanh} x&={\frac {1}{1-x^{2}}}&&|x|<1\\{\frac {d}{dx}}\operatorname {arcoth} x&={\frac {1}{1-x^{2}}}&&1<|x|\\{\frac {d}{dx}}\operatorname {arsech} x&=-{\frac {1}{x{\sqrt {1-x^{2}}}}}&&0<x<1\\{\frac {d}{dx}}\operatorname {arcsch} x&=-{\frac {1}{|x|{\sqrt {1+x^{2}}}}}&&x\neq 0\end{aligned}}}
Each of the functionssinh andcosh is equal to itssecond derivative ,that is:
d
2
d
x
2
sinh
x
=
sinh
x
{\displaystyle {\frac {d^{2}}{dx^{2}}}\sinh x=\sinh x}
d
2
d
x
2
cosh
x
=
cosh
x
.
{\displaystyle {\frac {d^{2}}{dx^{2}}}\cosh x=\cosh x\,.}
All functions with this property arelinear combinations ofsinh andcosh ,in particular theexponential functions
e
x
{\displaystyle e^{x}}
and
e
−
x
{\displaystyle e^{-x}}
.[ 22]
∫
sinh
(
a
x
)
d
x
=
a
−
1
cosh
(
a
x
)
+
C
∫
cosh
(
a
x
)
d
x
=
a
−
1
sinh
(
a
x
)
+
C
∫
tanh
(
a
x
)
d
x
=
a
−
1
ln
(
cosh
(
a
x
)
)
+
C
∫
coth
(
a
x
)
d
x
=
a
−
1
ln
|
sinh
(
a
x
)
|
+
C
∫
sech
(
a
x
)
d
x
=
a
−
1
arctan
(
sinh
(
a
x
)
)
+
C
∫
csch
(
a
x
)
d
x
=
a
−
1
ln
|
tanh
(
a
x
2
)
|
+
C
=
a
−
1
ln
|
coth
(
a
x
)
−
csch
(
a
x
)
|
+
C
=
−
a
−
1
arcoth
(
cosh
(
a
x
)
)
+
C
{\displaystyle {\begin{aligned}\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 \left|\sinh(ax)\right|+C\\\int \operatorname {sech} (ax)\,dx&=a^{-1}\arctan(\sinh(ax))+C\\\int \operatorname {csch} (ax)\,dx&=a^{-1}\ln \left|\tanh \left({\frac {ax}{2}}\right)\right|+C=a^{-1}\ln \left|\coth \left(ax\right)-\operatorname {csch} \left(ax\right)\right|+C=-a^{-1}\operatorname {arcoth} \left(\cosh \left(ax\right)\right)+C\end{aligned}}}
The following integrals can be proved usinghyperbolic substitution :
∫
1
a
2
+
u
2
d
u
=
arsinh
(
u
a
)
+
C
∫
1
u
2
−
a
2
d
u
=
sgn
u
arcosh
|
u
a
|
+
C
∫
1
a
2
−
u
2
d
u
=
a
−
1
artanh
(
u
a
)
+
C
u
2
<
a
2
∫
1
a
2
−
u
2
d
u
=
a
−
1
arcoth
(
u
a
)
+
C
u
2
>
a
2
∫
1
u
a
2
−
u
2
d
u
=
−
a
−
1
arsech
|
u
a
|
+
C
∫
1
u
a
2
+
u
2
d
u
=
−
a
−
1
arcsch
|
u
a
|
+
C
{\displaystyle {\begin{aligned}\int {{\frac {1}{\sqrt {a^{2}+u^{2}}}}\,du}&=\operatorname {arsinh} \left({\frac {u}{a}}\right)+C\\\int {{\frac {1}{\sqrt {u^{2}-a^{2}}}}\,du}&=\operatorname {sgn} {u}\operatorname {arcosh} \left|{\frac {u}{a}}\right|+C\\\int {\frac {1}{a^{2}-u^{2}}}\,du&=a^{-1}\operatorname {artanh} \left({\frac {u}{a}}\right)+C&&u^{2}<a^{2}\\\int {\frac {1}{a^{2}-u^{2}}}\,du&=a^{-1}\operatorname {arcoth} \left({\frac {u}{a}}\right)+C&&u^{2}>a^{2}\\\int {{\frac {1}{u{\sqrt {a^{2}-u^{2}}}}}\,du}&=-a^{-1}\operatorname {arsech} \left|{\frac {u}{a}}\right|+C\\\int {{\frac {1}{u{\sqrt {a^{2}+u^{2}}}}}\,du}&=-a^{-1}\operatorname {arcsch} \left|{\frac {u}{a}}\right|+C\end{aligned}}}
whereC is theconstant of integration .
Taylor series expressions [ edit ]
It is possible to express explicitly theTaylor series at zero (or theLaurent series ,if the function is not defined at zero) of the above functions.
sinh
x
=
x
+
x
3
3
!
+
x
5
5
!
+
x
7
7
!
+
⋯
=
∑
n
=
0
∞
x
2
n
+
1
(
2
n
+
1
)
!
{\displaystyle \sinh x=x+{\frac {x^{3}}{3!}}+{\frac {x^{5}}{5!}}+{\frac {x^{7}}{7!}}+\cdots =\sum _{n=0}^{\infty }{\frac {x^{2n+1}}{(2n+1)!}}}
This series isconvergent for everycomplex value ofx .Since the functionsinhx isodd ,only odd exponents forx occur in its Taylor series.
cosh
x
=
1
+
x
2
2
!
+
x
4
4
!
+
x
6
6
!
+
⋯
=
∑
n
=
0
∞
x
2
n
(
2
n
)
!
{\displaystyle \cosh x=1+{\frac {x^{2}}{2!}}+{\frac {x^{4}}{4!}}+{\frac {x^{6}}{6!}}+\cdots =\sum _{n=0}^{\infty }{\frac {x^{2n}}{(2n)!}}}
This series isconvergent for everycomplex value ofx .Since the functioncoshx iseven ,only even exponents forx occur in its Taylor series.
The sum of the sinh and cosh series is theinfinite series expression of theexponential function .
The following series are followed by a description of a subset of theirdomain of convergence ,where the series is convergent and its sum equals the function.
tanh
x
=
x
−
x
3
3
+
2
x
5
15
−
17
x
7
315
+
⋯
=
∑
n
=
1
∞
2
2
n
(
2
2
n
−
1
)
B
2
n
x
2
n
−
1
(
2
n
)
!
,
|
x
|
<
π
2
coth
x
=
x
−
1
+
x
3
−
x
3
45
+
2
x
5
945
+
⋯
=
∑
n
=
0
∞
2
2
n
B
2
n
x
2
n
−
1
(
2
n
)
!
,
0
<
|
x
|
<
π
sech
x
=
1
−
x
2
2
+
5
x
4
24
−
61
x
6
720
+
⋯
=
∑
n
=
0
∞
E
2
n
x
2
n
(
2
n
)
!
,
|
x
|
<
π
2
csch
x
=
x
−
1
−
x
6
+
7
x
3
360
−
31
x
5
15120
+
⋯
=
∑
n
=
0
∞
2
(
1
−
2
2
n
−
1
)
B
2
n
x
2
n
−
1
(
2
n
)
!
,
0
<
|
x
|
<
π
{\displaystyle {\begin{aligned}\tanh x&=x-{\frac {x^{3}}{3}}+{\frac {2x^{5}}{15}}-{\frac {17x^{7}}{315}}+\cdots =\sum _{n=1}^{\infty }{\frac {2^{2n}(2^{2n}-1)B_{2n}x^{2n-1}}{(2n)!}},\qquad \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}^{\infty }{\frac {2^{2n}B_{2n}x^{2n-1}}{(2n)!}},\qquad 0<\left|x\right|<\pi \\\operatorname {sech} x&=1-{\frac {x^{2}}{2}}+{\frac {5x^{4}}{24}}-{\frac {61x^{6}}{720}}+\cdots =\sum _{n=0}^{\infty }{\frac {E_{2n}x^{2n}}{(2n)!}},\qquad \left|x\right|<{\frac {\pi }{2}}\\\operatorname {csch} x&=x^{-1}-{\frac {x}{6}}+{\frac {7x^{3}}{360}}-{\frac {31x^{5}}{15120}}+\cdots =\sum _{n=0}^{\infty }{\frac {2(1-2^{2n-1})B_{2n}x^{2n-1}}{(2n)!}},\qquad 0<\left|x\right|<\pi \end{aligned}}}
where:
Infinite products and continued fractions [ edit ]
The following expansions are valid in the whole complex plane:
sinh
x
=
x
∏
n
=
1
∞
(
1
+
x
2
n
2
π
2
)
=
x
1
−
x
2
2
⋅
3
+
x
2
−
2
⋅
3
x
2
4
⋅
5
+
x
2
−
4
⋅
5
x
2
6
⋅
7
+
x
2
−
⋱
{\displaystyle \sinh x=x\prod _{n=1}^{\infty }\left(1+{\frac {x^{2}}{n^{2}\pi ^{2}}}\right)={\cfrac {x}{1-{\cfrac {x^{2}}{2\cdot 3+x^{2}-{\cfrac {2\cdot 3x^{2}}{4\cdot 5+x^{2}-{\cfrac {4\cdot 5x^{2}}{6\cdot 7+x^{2}-\ddots }}}}}}}}}
cosh
x
=
∏
n
=
1
∞
(
1
+
x
2
(
n
−
1
/
2
)
2
π
2
)
=
1
1
−
x
2
1
⋅
2
+
x
2
−
1
⋅
2
x
2
3
⋅
4
+
x
2
−
3
⋅
4
x
2
5
⋅
6
+
x
2
−
⋱
{\displaystyle \cosh x=\prod _{n=1}^{\infty }\left(1+{\frac {x^{2}}{(n-1/2)^{2}\pi ^{2}}}\right)={\cfrac {1}{1-{\cfrac {x^{2}}{1\cdot 2+x^{2}-{\cfrac {1\cdot 2x^{2}}{3\cdot 4+x^{2}-{\cfrac {3\cdot 4x^{2}}{5\cdot 6+x^{2}-\ddots }}}}}}}}}
tanh
x
=
1
1
x
+
1
3
x
+
1
5
x
+
1
7
x
+
⋱
{\displaystyle \tanh x={\cfrac {1}{{\cfrac {1}{x}}+{\cfrac {1}{{\cfrac {3}{x}}+{\cfrac {1}{{\cfrac {5}{x}}+{\cfrac {1}{{\cfrac {7}{x}}+\ddots }}}}}}}}}
Comparison with circular functions [ edit ]
Circle and hyperbola tangent at (1,1) display geometry of circular functions in terms ofcircular sector areau and hyperbolic functions depending onhyperbolic sector areau .
The hyperbolic functions represent an expansion oftrigonometry beyond thecircular functions .Both types depend on anargument ,eithercircular angle orhyperbolic angle .
Since thearea of a circular sector with radiusr and angleu (in radians) isr 2 u /2 ,it will be equal tou whenr =√2 .In the diagram, such a circle is tangent to the hyperbolaxy = 1 at (1,1). The yellow sector depicts an area and angle magnitude. Similarly, the yellow and red regions together depict ahyperbolic sector with area corresponding to hyperbolic angle magnitude.
The legs of the tworight triangles with hypotenuse on the ray defining the angles are of length√2 times the circular and hyperbolic functions.
The hyperbolic angle is aninvariant measure with respect to thesqueeze mapping ,just as the circular angle is invariant under rotation.[ 23]
TheGudermannian function gives a direct relationship between the circular functions and the hyperbolic functions that does not involve complex numbers.
The graph of the functiona cosh(x /a ) is thecatenary ,the curve formed by a uniform flexible chain, hanging freely between two fixed points under uniform gravity.
Relationship to the exponential function [ edit ]
The decomposition of the exponential function in itseven and odd parts gives the identities
e
x
=
cosh
x
+
sinh
x
,
{\displaystyle e^{x}=\cosh x+\sinh x,}
and
e
−
x
=
cosh
x
−
sinh
x
.
{\displaystyle e^{-x}=\cosh x-\sinh x.}
Combined withEuler's formula
e
i
x
=
cos
x
+
i
sin
x
,
{\displaystyle e^{ix}=\cos x+i\sin x,}
this gives
e
x
+
i
y
=
(
cosh
x
+
sinh
x
)
(
cos
y
+
i
sin
y
)
{\displaystyle e^{x+iy}=(\cosh x+\sinh x)(\cos y+i\sin y)}
for thegeneral complex exponential function .
Additionally,
e
x
=
1
+
tanh
x
1
−
tanh
x
=
1
+
tanh
x
2
1
−
tanh
x
2
{\displaystyle 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 [ edit ]
Hyperbolic functions in the complex plane
sinh
(
z
)
{\displaystyle \sinh(z)}
cosh
(
z
)
{\displaystyle \cosh(z)}
tanh
(
z
)
{\displaystyle \tanh(z)}
coth
(
z
)
{\displaystyle \coth(z)}
sech
(
z
)
{\displaystyle \operatorname {sech} (z)}
csch
(
z
)
{\displaystyle \operatorname {csch} (z)}
Since theexponential function can be defined for anycomplex argument, we can also extend the definitions of the hyperbolic functions to complex arguments. The functionssinhz andcoshz are thenholomorphic .
Relationships to ordinary trigonometric functions are given byEuler's formula for complex numbers:
e
i
x
=
cos
x
+
i
sin
x
e
−
i
x
=
cos
x
−
i
sin
x
{\displaystyle {\begin{aligned}e^{ix}&=\cos x+i\sin x\\e^{-ix}&=\cos x-i\sin x\end{aligned}}}
so:
cosh
(
i
x
)
=
1
2
(
e
i
x
+
e
−
i
x
)
=
cos
x
sinh
(
i
x
)
=
1
2
(
e
i
x
−
e
−
i
x
)
=
i
sin
x
cosh
(
x
+
i
y
)
=
cosh
(
x
)
cos
(
y
)
+
i
sinh
(
x
)
sin
(
y
)
sinh
(
x
+
i
y
)
=
sinh
(
x
)
cos
(
y
)
+
i
cosh
(
x
)
sin
(
y
)
tanh
(
i
x
)
=
i
tan
x
cosh
x
=
cos
(
i
x
)
sinh
x
=
−
i
sin
(
i
x
)
tanh
x
=
−
i
tan
(
i
x
)
{\displaystyle {\begin{aligned}\cosh(ix)&={\frac {1}{2}}\left(e^{ix}+e^{-ix}\right)=\cos x\\\sinh(ix)&={\frac {1}{2}}\left(e^{ix}-e^{-ix}\right)=i\sin 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(ix)&=i\tan x\\\cosh x&=\cos(ix)\\\sinh x&=-i\sin(ix)\\\tanh x&=-i\tan(ix)\end{aligned}}}
Thus, hyperbolic functions areperiodic with respect to the imaginary component, with period
2
π
i
{\displaystyle 2\pi i}
(
π
i
{\displaystyle \pi i}
for hyperbolic tangent and cotangent).
^a b c d Weisstein, Eric W."Hyperbolic Functions" .mathworld.wolfram .Retrieved2020-08-29 .
^ (1999)Collins Concise Dictionary ,4th edition, HarperCollins, Glasgow,ISBN 0 00 472257 4 ,p. 1386
^a b Collins Concise Dictionary ,p. 328
^a b "Hyperbolic Functions" .mathsisfun .Retrieved2020-08-29 .
^ Collins Concise Dictionary ,p. 1520
^ Collins Concise Dictionary ,p. 329
^ tanh
^ Collins Concise Dictionary ,p. 1340
^ Woodhouse, N. M. J. (2003),Special Relativity ,London: Springer, p. 71,ISBN 978-1-85233-426-0
^ Abramowitz, Milton ;Stegun, Irene A. ,eds. (1972),Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables ,New York:Dover Publications ,ISBN 978-0-486-61272-0
^ Some examples of usingarcsinh found inGoogle Books .
^ Niven, Ivan (1985).Irrational Numbers .Vol. 11. Mathematical Association of America.ISBN 9780883850381 .JSTOR 10.4169/j.ctt5hh8zn .
^ Robert E. Bradley, Lawrence A. D'Antonio, Charles Edward Sandifer.Euler at 300: an appreciation. Mathematical Association of America, 2007. Page 100.
^ Georg F. Becker.Hyperbolic functions. Read Books, 1931. Page xlviii.
^ N.P., Bali (2005).Golden Integral Calculus .Firewall Media. p. 472.ISBN 81-7008-169-6 .
^ Willi-hans Steeb (2005).Nonlinear Workbook, The: Chaos, Fractals, Cellular Automata, Neural Networks, Genetic Algorithms, Gene Expression Programming, Support Vector Machine, Wavelets, Hidden Markov Models, Fuzzy Logic With C++, Java And Symbolicc++ Programs (3rd ed.). World Scientific Publishing Company. p. 281.ISBN 978-981-310-648-2 . Extract of page 281 (using lambda=1)
^ Keith B. Oldham; Jan Myland; Jerome Spanier (2010).An Atlas of Functions: with Equator, the Atlas Function Calculator (2nd, illustrated ed.). Springer Science & Business Media. p. 290.ISBN 978-0-387-48807-3 . Extract of page 290
^ Osborn, G. (July 1902)."Mnemonic for hyperbolic formulae" .The Mathematical Gazette .2 (34): 189.doi :10.2307/3602492 .JSTOR 3602492 .S2CID 125866575 .
^ Martin, George E. (1986).The foundations of geometry and the non-euclidean plane (1st corr. ed.). New York: Springer-Verlag. p. 416.ISBN 3-540-90694-0 .
^ "Prove the identity tanh(x/2) = (cosh(x) - 1)/sinh(x)" .StackExchange (mathematics).Retrieved24 January 2016 .
^ Audibert, Jean-Yves (2009). "Fast learning rates in statistical inference through aggregation". The Annals of Statistics. p. 1627. [1]
^ Olver, Frank W. J. ;Lozier, Daniel M.; Boisvert, Ronald F.; Clark, Charles W., eds. (2010),"Hyperbolic functions" ,NIST Handbook of Mathematical Functions ,Cambridge University Press,ISBN 978-0-521-19225-5 ,MR 2723248 .
^ Mellen W. Haskell ,"On the introduction of the notion of hyperbolic functions",Bulletin of the American Mathematical Society 1 :6:155–9,full text
Trigonometric and hyperbolic functions
Groups Other