Hyperbolic Functions

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The hyperbolic functions sinhz, coshz, tanhz, cschz, sechz, cothz (hyperbolic sine, hyperbolic cosine, hyperbolic tangent, hyperbolic cosecant, hyperbolic secant, and hyperbolic cotangent) are analogs of the circular functions, defined by removing is appearing in the complex exponentials. For example,

 cosz=1/2(e^(iz)+e^(-iz)),
(1)

so

 coshz=1/2(e^z+e^(-z)).
(2)

Note that alternate notations are sometimes used, as summarized in the following table.

f(x)alternate notations
coshzchz (Gradshteyn and Ryzhik 2000, p. xxvii)
cothzcthz (Gradshteyn and Ryzhik 2000, p. xxvii)
sinhzshz (Gradshteyn and Ryzhik 2000, p. xxvii)
tanhzthz (Gradshteyn and Ryzhik 2000, p. xxvii)

The hyperbolic functions share many properties with the corresponding circular functions. In fact, just as the circle can be represented parametrically by

x=acost
(3)
y=asint,
(4)

a rectangular hyperbola (or, more specifically, its right branch) can be analogously represented by

x=acosht
(5)
y=asinht,
(6)

where cosht is the hyperbolic cosine and sinht is the hyperbolic sine.

The hyperbolic functions arise in many problems of mathematics and mathematical physics in which integrals involving sqrt(1+x^2) arise (whereas the circular functions involve sqrt(1-x^2)). For instance, the hyperbolic sine arises in the gravitational potential of a cylinder and the calculation of the Roche limit. The hyperbolic cosine function is the shape of a hanging cable (the so-called catenary). The hyperbolic tangent arises in the calculation of and rapidity of special relativity. All three appear in the Schwarzschild metric using external isotropic Kruskal coordinates in general relativity. The hyperbolic secant arises in the profile of a laminar jet. The hyperbolic cotangent arises in the Langevin function for magnetic polarization.

The hyperbolic functions are defined by

sinhz=(e^z-e^(-z))/2
(7)
=-sinh(-z)
(8)
coshz=(e^z+e^(-z))/2
(9)
=cosh(-z)
(10)
tanhz=(e^z-e^(-z))/(e^z+e^(-z))
(11)
=(e^(2z)-1)/(e^(2z)+1)
(12)
cschz=2/(e^z-e^(-z))
(13)
sechz=2/(e^z+e^(-z))
(14)
cothz=(e^z+e^(-z))/(e^z-e^(-z))
(15)
=(e^(2z)+1)/(e^(2z)-1).
(16)

For arguments multiplied by i,

 sinh(iz)=isinz
(17)
 cosh(iz)=cosz.
(18)

The hyperbolic functions satisfy many identities analogous to the trigonometric identities (which can be inferred using Osborn's rule) such as

cosh^2x-sinh^2x=1
(19)
coshx+sinhx=e^x
(20)
coshx-sinhx=e^(-x).
(21)

See also Beyer (1987, p. 168).

Some half-angle formulas are

tanh(z/2)=(sinhx+isiny)/(coshx+cosy)
(22)
coth(z/2)=(sinhx-isiny)/(coshx-cosy),
(23)

where z=x+iy.

Some double-angle formulas are

sinh(2z)=2sinhzcoshz
(24)
cosh(2z)=2cosh^2z-1
(25)
=1+2sinh^2z.
(26)

Identities for complex arguments include

sinh(x+iy)=sinhxcosy+icoshxsiny
(27)
cosh(x+iy)=coshxcosy+isinhxsiny.
(28)

The absolute squares for complex arguments are

|sinh(z)|^2=sinh^2x+sin^2y
(29)
|cosh(z)|^2=sinh^2x+cos^2y.
(30)

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