Calculating a Motion Integral Without Hyperbolic Trigonometry

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[tex]\int \frac{dx} { \sqrt{ \frac{1}{x} - \frac{1}{b}} }[/tex]
where b is a positive constant.
Using http://integrals.wolfram.com" , I know the result:
[tex]-\sqrt{bx} \sqrt{b-x} + b\sqrt{b} \tan^{-1}( \frac{\sqrt{x}} {\sqrt{b-x}})[/tex]
but how do I calculate it from scratch?
 
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I'd substitute

[tex] \frac{1}{x} - \frac{1}{b} = y^2 \Leftrightarrow \frac{1}{x} = y^2 + \frac{1}{b} \Leftrightarrow x = \frac{b}{{by^2 + 1}} \Leftrightarrow dx = \frac{{ - b^2 y}}{{\left( {by^2 + 1} \right)^2 }}[/tex]

It gets rid of the square root and returns a rational function in y.
 
After a few conversions, I ended up with this
[tex]C \int \frac{du}{(u^2 + 1)^2}[/tex]
Which I couldn't solve. I tried switching
[tex]u = \sinh(t), du = \cosh(t)dt[/tex]
and
[tex]\int \frac{dt}{\cosh^3(t)}[/tex]
but got stuck again.
 
Got it done. Thanks!
 
gulsen said:
Got it done. Thanks!
You're welcome!
 
The way i see it, there's no need for hyperbolic trigonometry.

[tex]\int \frac{\sqrt{bx}}{\sqrt{b-x}} \ dx[/tex]

becomes under the substitution [tex]\sqrt{x} =\sqrt{b} \sin t[/tex]

an integral ~ to [itex]\int \sin^{2} t \ dt[/itex].

Daniel.