Computing the length of the polar curve $r = \frac{2}{\theta}$ using a hyperbolic substitution $$\begin{align}
L&:=\int_{\theta_1}^{\theta_2}\sqrt{\left({\mathrm{d}x\over\mathrm{d}\theta}\right)^2+\left({\mathrm{d}y\over\mathrm{d}\theta}\right)^2}\,\mathrm{d}\theta
\\\\r&:={2\over\theta}
\\
&\begin{cases}
\theta_1=1/2\\\theta_2=4
\end{cases}
\\&\begin{cases}
x=r\cos(\theta)\\y=r\sin(\theta)
\end{cases}
\\
L&=\int_{{1\over 2}}^{4}\sqrt{\left({\mathrm{d}x\over\mathrm{d}\theta}\right)^2+\left({\mathrm{d}y\over\mathrm{d}\theta}\right)^2}\,\mathrm{d}\theta
\end{align}$$
The problem above is from this book(A First Course in Calculus by Serge Lang)
The book says use $~\theta=\sinh(t)~$as a hint.
I tried to find out$~L~$without using that substitution of variable, but failed to.
So I am now willing to use$~\theta=\sinh(t)~$
$$\begin{align}
t&:=\sinh^{-1}(\theta)\implies \theta=\sinh(t)\\
{\mathrm{d} \theta \over \mathrm{d} t }&=\cosh(t)
\\x&= {2 \over \theta }\cos(\theta)\\
y&= {2 \over \theta }\sin(\theta)
\end{align}$$
Stucked from here.
How can I handle trigonometric functions with hyperbolic functions in this case?
 A: Substituting the formulas for $x, y$ in the arc length formula and simplifying gives
$$L = 2 \int_\frac{1}{2}^4 \frac{\sqrt{1 + \theta^2}}{\theta^2} \,d\theta ;$$ notice that trigonometric functions do not appear in the integrand. (Remark It's easier to arrive at this formula using the equation for arc length of a polar curve $r(\theta)$, namely, $\int_a^b \sqrt{r^2 + \left(\frac{dr}{d\theta}\right)^2}\,d\theta$.)
At this point, the appearance of the factor $\sqrt{1 + \theta^2}$ suggests the substitution $$\theta = \sinh t, \qquad d\theta = \cosh t\,dt ,$$ since $\sqrt{(\sinh t)^2 + 1} = \cosh t$, which transforms the integral to
$$2 \int_{\operatorname{arsinh} \frac{1}{2}}^{\operatorname{arsinh} 4} \coth^2 t \,dt = t - \coth t \Bigg\vert_{\operatorname{arsinh} \frac{1}{2}}^{\operatorname{arsinh} 4}.$$ To simplify the resulting expression it will be helpful to recall the identity $\coth \operatorname{arsinh} \theta = \frac{\sqrt{1 + \theta^2}}{\theta}$.
Remark You might find the original integral easier to evaluating using the similar substitution $\theta = \tan \alpha$, $d\theta = \sec^2 \alpha \,d\alpha$, which yields
$$2 \int_{\arctan \frac{1}{2}}^{\arctan 4} \frac{d\alpha}{\sin^2 \alpha \cos \alpha} .$$
