1.175201
2.718282
0.367879
1.543081
0.761594
1.175201
2.718282
0.367879
1.543081
0.761594
The Hyperbolic Sine Calculator computes $$\sinh(x)$$ for any real number $$x$$. The hyperbolic sine function is one of the six hyperbolic functions, which are analogs of the ordinary trigonometric functions but based on hyperbolas rather than circles.
The hyperbolic sine is defined by the exponential formula:
$$\sinh(x) = \frac{e^x - e^{-x}}{2}$$
where $$e \approx 2.71828$$ is Euler's number. This formula shows that $$\sinh(x)$$ is the difference of two exponential curves, scaled by one-half. For large positive $$x$$, the $$e^x$$ term dominates and $$\sinh(x) \approx \frac{e^x}{2}$$. For large negative $$x$$, the $$e^{-x}$$ term dominates and $$\sinh(x) \approx -\frac{e^{-x}}{2}$$.
Just as $$\cos(t)$$ and $$\sin(t)$$ parametrize the unit circle $$x^2 + y^2 = 1$$, the hyperbolic functions $$\cosh(t)$$ and $$\sinh(t)$$ parametrize the right branch of the unit hyperbola:
$$\cosh^2(t) - \sinh^2(t) = 1$$
This identity is the hyperbolic analog of the Pythagorean identity $$\cos^2(t) + \sin^2(t) = 1$$.
Through Euler's formula, the hyperbolic sine relates to the ordinary sine function in the complex plane:
$$\sinh(x) = -i\sin(ix)$$
This connection shows that hyperbolic functions are essentially trigonometric functions with imaginary arguments.
The hyperbolic sine appears naturally in many physical and engineering contexts. The catenary curve — the shape of a hanging chain or cable under uniform gravity — is described by $$y = a\cosh\left(\frac{x}{a}\right)$$, with the vertical component of tension involving $$\sinh$$. In electrical engineering, the transmission line equations use $$\sinh$$ and $$\cosh$$ to model voltage and current distribution along long cables. In special relativity, $$\sinh$$ parametrizes the rapidity, which is the hyperbolic analog of velocity angle. In heat transfer, solutions to the heat equation in finite domains involve hyperbolic sines. The function also appears in the solutions to Laplace's equation in rectangular coordinates and in the deflection formulas for beams and plates.
Enter a real number $$x$$. The calculator evaluates $$\sinh(x) = \frac{e^x - e^{-x}}{2}$$ and also displays the intermediate values $$e^x$$ and $$e^{-x}$$ for reference.
The result $$\sinh(x)$$ grows exponentially for large $$|x|$$. For small values near zero, $$\sinh(x) \approx x$$. The function passes through the origin and is strictly increasing, making it invertible over its entire domain.
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sinh(1) = (e¹ − e⁻¹)/2 = (2.71828 − 0.36788)/2 ≈ 1.17520.
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Since sinh is an odd function, sinh(−2) = −sinh(2) ≈ −3.62686.
The 'h' stands for hyperbolic. The function $$\sinh$$ is the hyperbolic analog of the circular sine function $$\sin$$. While sine and cosine parametrize a circle, hyperbolic sine and cosine parametrize a hyperbola.
No. $$\sin(x)$$ is the circular sine function, bounded between -1 and 1 and periodic. $$\sinh(x)$$ is the hyperbolic sine, which is unbounded and not periodic. For small $$x$$, they are approximately equal ($$\sinh(x) \approx \sin(x) \approx x$$), but they diverge rapidly for larger values.
The inverse hyperbolic sine is $$\text{arcsinh}(x) = \ln\left(x + \sqrt{x^2 + 1}\right)$$, sometimes written as $$\sinh^{-1}(x)$$. Unlike the inverse circular functions, arcsinh is defined for all real numbers.
For large $$x$$, $$\sinh(x) \approx \frac{e^x}{2}$$, which grows exponentially. The $$e^{-x}$$ term becomes negligible. For example, $$\sinh(10) \approx 11013$$, while $$\sin(10) \approx -0.544$$.
The fundamental identity is $$\cosh^2(x) - \sinh^2(x) = 1$$, analogous to $$\cos^2(x) + \sin^2(x) = 1$$. Other useful identities include the double-angle formula: $$\sinh(2x) = 2\sinh(x)\cosh(x)$$.
The hyperbolic sine appears in catenary curves (hanging cables), transmission line theory, special relativity (rapidity), solutions to Laplace's equation, and beam deflection formulas. It arises naturally wherever exponential growth and decay combine symmetrically.
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