Introduction
The geometric construction of the hyperbolic sine, based on the area of a sector of the equilateral hyperbola, appears in hyperbolic sine and cosine. For real $x,$ the hyperbolic sine is the function defined by the exponential formula:
$$\sinh(x) = \frac{e^x - e^{-x}}{2}$$
The function $f(x) = \sinh(x)$ is half the difference of $e^x$ and $e^{-x}.$ It is defined for every real number and has range $\mathbb{R}.$ Its graph is symmetric about the origin and has tangent $y = x$ at the point $(0, 0).$ The function tends to $+\infty$ as $x \to +\infty$ and to $-\infty$ as $x \to -\infty,$ while the circular sine oscillates. For large positive $x,$ the term $e^{-x}$ is close to zero and $\sinh(x)$ is close to $e^x/2.$ By oddness, $\sinh(x)$ is close to $-e^{-x}/2$ for large negative $x.$
The hyperbolic sine gives the arc length of the catenary $y = \cosh(x),$ along which a uniform chain hangs under its own weight. For $a \geq 0,$ the length of the arc from the vertex to the point of abscissa $a$ is $\sinh(a).$
Properties
The function has the following properties.
- Domain: $x \in \mathbb{R}$
- Range: $y \in \mathbb{R}$
- Periodicity: not periodic
- Parity: odd, with $\sinh(-x) = -\sinh(x)$
- Monotonicity: strictly increasing on $\mathbb{R}$
- Sign: negative on $(-\infty, 0),$ zero at $x = 0,$ and positive on $(0, +\infty)$
- Roots: $x = 0$
- Maximum and minimum points: the function has none and is unbounded above and below.
The hyperbolic sine and the hyperbolic cosine satisfy the fundamental hyperbolic identity:
$$\cosh^2(x) - \sinh^2(x) = 1$$
Since $\cosh(x)$ is positive for every real $x,$ solving the hyperbolic identity for $\cosh(x)$ gives:
$$\cosh(x) = \sqrt{1 + \sinh^2(x)}$$
Every real value has exactly one preimage, so the hyperbolic sine is a bijection of $\mathbb{R}$ onto $\mathbb{R}.$
Limits, derivatives, and integrals of the hyperbolic sine function
The remarkable limit of the exponential function determines the behaviour near the origin. The relevant quotient is:
$$\frac{\sinh(x)}{x} = \frac{1}{2}\left(\frac{e^x - 1}{x} + \frac{e^{-x} - 1}{-x}\right)$$
As $x$ tends to zero, both quotients in parentheses tend to $1.$ Their half-sum tends to one:
$$\lim_{x \to 0} \frac{\sinh(x)}{x} = 1$$
Near the origin, both $\sinh(x)$ and $\sin(x)$ are close to $x.$ The limits at infinity and the comparison with $e^x/2$ at $+\infty$ are:
$$ \begin{align} \lim_{x \to +\infty} \sinh(x) &= +\infty \\[6pt] \lim_{x \to -\infty} \sinh(x) &= -\infty \\[6pt] \lim_{x \to +\infty} \left(\sinh(x) - \frac{e^x}{2}\right) &= 0 \end{align} $$
The equality $\sinh(x) - e^x/2 = -e^{-x}/2$ shows that the curve approaches $e^x/2$ from below at $+\infty.$ At $-\infty,$ the equality $\sinh(x) + e^{-x}/2 = e^x/2 \to 0$ shows that the curve approaches $-e^{-x}/2$ from above. The graph has no vertical asymptotes because it is continuous on $\mathbb{R}.$ Since $\dfrac{\sinh(x)}{x} \to +\infty$ as $x \to \pm\infty,$ it has no horizontal or oblique asymptotes.
The function $\sinh(x)$ is continuous and differentiable on $\mathbb{R}.$ Termwise differentiation of the exponential expression gives its derivative:
$$\frac{d}{dx}\sinh(x) = \frac{e^x + e^{-x}}{2} = \cosh(x)$$
A second differentiation returns the original function, so the derivatives alternate with period two:
$$\frac{d^2}{dx^2}\sinh(x) = \sinh(x)$$
The parity of $n$ determines the $n$-th derivative:
$$ \frac{d^n}{dx^n}\sinh(x) = \begin{cases} \sinh(x) & \text{if } n \text{ is even} \\[6pt] \cosh(x) & \text{if } n \text{ is odd} \end{cases} $$
The hyperbolic sine is the unique solution of the differential equation $y'' = y$ with $y(0) = 0$ and $y'(0) = 1.$ The circular sine solves $y'' = -y$ with the same initial conditions.
The indefinite integral of the hyperbolic sine is:
$$\int \sinh(x) \ dx = \cosh(x) + c$$
Because the function is odd, its definite integral over an interval symmetric about the origin vanishes:
$$\int_{-a}^{a} \sinh(x) \ dx = 0$$
For the catenary $y = \cosh(x),$ the derivative satisfies $y'(x) = \sinh(x),$ and the fundamental hyperbolic identity gives $\sqrt{1 + [y'(x)]^2} = \cosh(x).$ The arc-length formula therefore yields $\int_0^a \cosh(x) \ dx = \sinh(a)$ for $a \geq 0.$
For integrals containing $\sqrt{1 + x^2},$ the substitution $x = \sinh(t)$ gives $\sqrt{1 + x^2} = \cosh(t)$ and $dx = \cosh(t) \ dt,$ so the radical disappears. The trigonometric substitution for $\sqrt{1 - x^2}$ is $x = \sin(t)$ with $-\pi/2 \leq t \leq \pi/2.$
Monotonicity and convexity
The derivative $\cosh(x)$ is at least $1$ at every point, so the hyperbolic sine is strictly increasing on $\mathbb{R}$ and has no stationary points. Equality holds only at $x = 0,$ where the tangent is the line $y = x.$ Thus the smallest slope is $1.$
Since $\sinh''(x) = \sinh(x)$ is negative for $x < 0$ and positive for $x > 0,$ the graph is strictly concave on $(-\infty, 0)$ and strictly convex on $(0, +\infty).$ The origin is an inflection point, where the second derivative vanishes and changes sign.
Inverse function
The hyperbolic sine is continuous and strictly increasing, with range $\mathbb{R}.$ It is a bijection of $\mathbb{R}$ onto $\mathbb{R},$ and its inverse function is denoted by:
$$\mathrm{arsinh} : \mathbb{R} \to \mathbb{R}$$
With $t = e^y,$ the equation $x = \sinh(y)$ becomes $2x = t - t^{-1},$ which is equivalent to the quadratic equation:
$$t^2 - 2xt - 1 = 0$$
Its roots are $t = x \pm \sqrt{x^2 + 1}.$ Since $\sqrt{x^2 + 1} > |x|,$ only the root with the plus sign satisfies $t = e^y,$ because $e^y$ is positive. Taking the natural logarithm gives:
$$\mathrm{arsinh}(x) = \ln\left(x + \sqrt{x^2 + 1}\right)$$
For every real $x,$ the positivity of $\cosh$ and the fundamental hyperbolic identity give $\cosh(\mathrm{arsinh}(x)) = \sqrt{1 + x^2},$ so the derivative of the inverse function is:
$$\frac{d}{dx}\mathrm{arsinh}(x) = \frac{1}{\sqrt{1 + x^2}}$$
On $\mathbb{R},$ the antiderivatives of $\dfrac{1}{\sqrt{1 + x^2}}$ are:
$$\int \frac{1}{\sqrt{1 + x^2}} \ dx = \ln\left(x + \sqrt{x^2 + 1}\right) + c$$
Maclaurin series
The Maclaurin series of the hyperbolic sine follows from the series of the exponential function. Subtracting the expansion of $e^{-x}$ from that of $e^x$ cancels the even powers and doubles the odd powers. Dividing by $2$ gives a power series that converges for every real number:
$$\sinh(x) = \sum_{n=0}^{\infty} \frac{x^{2n+1}}{(2n+1)!} = x + \frac{x^3}{3!} + \frac{x^5}{5!} + \frac{x^7}{7!} + \cdots$$
Near the origin, the first term gives the linear approximation $y = x.$
For complex $x,$ replacing $x$ by $ix$ multiplies each term of degree $2n + 1$ by $i^{2n+1} = i(-1)^n,$ so $\sinh(ix) = i\sin(x).$ Applying this identity to $ix$ and using oddness gives $\sin(ix) = i\sinh(x).$
From the outset, Algebrica has been committed to full transparency about the editorial process behind the entries in its knowledge base. As an additional measure, readers can inspect the authorship assessment for each entry. For some translated content, the verification link points to the original Italian version, since translation and editing tools (including Grammarly, CoWork, and Claude) can introduce changes that affect the score. This assessment is provided as a transparency aid and should not be regarded as definitive proof of authorship.