y=sinh⁡xy = \sinh x

Graph of the Hyperbolic Sine y=sinh⁡xy = \sinh x

The hyperbolic sine function y=sinh⁡xy = \sinh x is defined in terms of the exponential function1.

sinh⁡x=ex−e−x2\sinh x = \frac{e^x - e^{-x}}{2}

It is the hyperbolic counterpart of the ordinary sine sin⁡x\sin x.

Domain and range

  • The domain is all real numbers
  • The range is all real numbers
  • It increases monotonically
  • It is an odd function

Being built from the difference of exe^x and e−xe^{-x}, it has a value at every real number. Unlike the sine, its values are not bounded, and that is the sharpest difference between the two.

Symmetry

Since sinh⁡(−x)=e−x−ex2=−sinh⁡x\sinh(-x) = \dfrac{e^{-x} - e^{x}}{2} = -\sinh x, the function is odd and its graph is symmetric about the origin.

Monotonicity

The derivative is ddxsinh⁡x=cosh⁡x\dfrac{d}{dx}\sinh x = \cosh x. Since cosh⁡x\cosh x is always at least 11, and therefore positive, sinh⁡x\sinh x is strictly increasing on the whole real line and has no extrema.

The second derivative is sinh⁡x\sinh x itself, so it changes sign only at the origin. The single inflection point is (0,0)(0, 0), where the curve turns from concave down to concave up.

Relation to the exponential

cosh⁡x+sinh⁡x=excosh⁡x−sinh⁡x=e−x\begin{align*} \cosh x + \sinh x &= e^x \\ \cosh x - \sinh x &= e^{-x} \end{align*}

One may read cosh⁡\cosh and sinh⁡\sinh as the even and the odd parts into which the exponential function splits.

Near the origin and far out

RangeApproximationBehavior
near the originsinh⁡x≈x\sinh x \approx xtangent to the line y=xy = x
x→+∞x \to +\inftysinh⁡x≈ex2\sinh x \approx \dfrac{e^x}{2}grows exponentially
x→−∞x \to -\inftysinh⁡x≈−e−x2\sinh x \approx -\dfrac{e^{-x}}{2}falls exponentially

There are no horizontal asymptotes. The Taylor series has only odd powers.

sinh⁡x=x+x33!+x55!+⋯\sinh x = x + \frac{x^3}{3!} + \frac{x^5}{5!} + \cdots

The coefficients have the same magnitudes as those of sin⁡x\sin x; only the alternation of signs is missing.

Notable values

xxsinh⁡x\sinh x
0000
11≈1.1752\approx 1.1752
22≈3.6269\approx 3.6269
33≈10.0179\approx 10.0179

Relation to the hyperbola

With the hyperbolic cosine it satisfies the identity cosh⁡2x−sinh⁡2x=1\cosh^2 x - \sinh^2 x = 1, from which the point (cosh⁡t,sinh⁡t)(\cosh t, \sinh t) always lies on the hyperbola x2−y2=1x^2 - y^2 = 1.

ItemTrigonometricHyperbolic
Identitycos⁡2t+sin⁡2t=1\cos^2 t + \sin^2 t = 1cosh⁡2t−sinh⁡2t=1\cosh^2 t - \sinh^2 t = 1
Curve the point lies onthe unit circlethe unit hyperbola
Derivative on the sine sidecos⁡t\cos tcosh⁡t\cosh t
Derivative on the cosine side−sin⁡t-\sin tsinh⁡t\sinh t
Period2π2\pinone

This corresponds to the fact that (cos⁡t,sin⁡t)(\cos t, \sin t) lies on the unit circle, and it is the origin of the name hyperbolic functions.

Applications

  • The catenary, the shape a chain or a cable takes under its own weight
  • The equations of a vibrating string and of heat conduction
  • The addition of velocities in special relativity, through rapidity2
  1. Hyperbolic functions, Wikipedia
  2. Rapidity, Wikipedia