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Let $H_1$ be the branch (connected component) of the unit hyperbola $x^2-y^2=1$ with $x>0$ .
unit=1.5cm
![\begin{pspicture}(-1,-2.25)(2.5,2.25) \psaxes[Dx=10,Dy=10]{<->}(0,0)(-1,-2.25)(2... ...xp -1 add 0.5 exp -1 mul} \rput[r](-1,0){.} \rput[a](0,-2.25){.} \end{pspicture} \begin{pspicture}(-1,-2.25)(2.5,2.25) \psaxes[Dx=10,Dy=10]{<->}(0,0)(-1,-2.25)(2... ...xp -1 add 0.5 exp -1 mul} \rput[r](-1,0){.} \rput[a](0,-2.25){.} \end{pspicture}](http://images.planetmath.org:8080/cache/objects/10390/js/img1.png)
Let $\alpha>0$ . Then $(\cosh\alpha,\sinh\alpha)$ is the point on $H_1$ with hyperbolic angle $\alpha$ .
In order to draw the hyperbolic angle, the line passing through $(0,0)$ and $(\cosh\alpha,\sinh\alpha)$ must be drawn. Recall that $\tanh\alpha$ is defined by$$ \tanh\alpha :=\frac{\sinh\alpha}{\cosh\alpha}.$$ Thus, the equation of the line passing through $(0,0)$ and $(\cosh\alpha,\sinh\alpha)$ is $y=(\tanh\alpha)x$ .
Below is the graph of $H_1$ and the line $y=(\tanh\alpha)x$ .
unit=2cm
![\begin{pspicture}(-1,-2.25)(2.5,2.25) \psaxes[Dx=10,Dy=10]{<->}(0,0)(-1,-2.25)(2... ...<->}(-1,-0.667)(1.95,1.3) \rput[r](-1,0){.} \rput[a](0,-2.25){.} \end{pspicture} \begin{pspicture}(-1,-2.25)(2.5,2.25) \psaxes[Dx=10,Dy=10]{<->}(0,0)(-1,-2.25)(2... ...<->}(-1,-0.667)(1.95,1.3) \rput[r](-1,0){.} \rput[a](0,-2.25){.} \end{pspicture}](http://images.planetmath.org:8080/cache/objects/10390/js/img2.png)
Observe also that $\sinh\alpha>0$ and $\cosh\alpha>1$ .
In the hyperbolic angle entry, it is discussed that $\alpha$ is twice the area bounded by the $x$ axis, $H_1$ , and the line $y=(\tanh\alpha)x$ . We will use this fact to obtain formulas for $\cosh\alpha$ and $\sinh\alpha$ .
In the calculations below, the following integration formula will be used: $$ \int\sqrt{x^2-1} \, dx=\frac{x}{2}\sqrt{x^2-1}-\frac{1}{2}\ln\left|x+\sqrt{x^2-1}\right|+C$$
Thus, we have
Thus, we have$$ e^{\alpha}=\cosh\alpha+\sinh\alpha.$$ A similar calculation yields$$ e^{-\alpha}=\cosh\alpha-\sinh\alpha.$$ The formulas for the hyperbolic functions are easily derived from the above equations:
As mentioned in the hyperbolic angle entry, these formulas can be extended to all $\alpha\in\mathbb{R}$ and from there to all $\alpha\in\mathbb{C}$ .
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