Prove that the integral is equal to ##\pi^2/8##

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The integral $$I = \int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx$$ is proposed to equal $$\frac{\pi^2}{8}.$$ The discussion involves using the representation of the arcsine function and applying Fubini's Theorem to interchange the order of integration, allowing for a transformation of the integral into a double integral. Participants explore various substitutions, including trigonometric substitutions, to simplify the integrand and compute the integral more effectively. The complexity of the integral and the challenge of finding closed-form solutions for the limits of integration are highlighted, with suggestions for further simplification and exploration of the integral's properties.
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Homework Statement
Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$
Relevant Equations
Fubini's Theorem, arcsin representation integral.
Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$

Let $$I = \int\limits_0^{\sqrt 2 / 4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx. \tag{1}$$

The representation integral of ##\arcsin## is $$\arcsin u = \int\limits_{0}^{1} \frac{\mathrm dt}{\sqrt{1-t^2}}, \qquad 0 \leqslant u \leqslant 1.$$
Plugging identity above into ##(1)## with ##u = \sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}##, we obtain
$$I = \int\limits_0^{\frac{\sqrt{2}}{4}} \frac{1}{\sqrt{x - x^2}} \int_0^{\sqrt{\frac{\left(x - 1\right) \left( x - 1 + \sqrt{9 - 16x} \right)}{1-2x}}} \frac{\mathrm dt}{\sqrt{1 - t^2}} \, \mathrm dx.$$
Since the integrand is non-negative and continuous over the rectangular domain ##D := \left\{(x, t) : 0 \leq x \leq \frac{\sqrt{2}}{4}, \,\, 0 \leq t \leq f(x)\right\}## (##f(x)## is the root of the numerator), Fubini's Theorem allows us to interchange the order:
$$I = \int\limits_0^1 \frac{\mathrm dt}{\sqrt{1 - t^2}} \int\limits_{x_*(t)}^{x^*(t)} \frac{\mathrm dx}{\sqrt{x- x^2}},$$
where ##x_*(t)## and ##x^*(t)## are the closed solutions of the equation
$$t^2 = \frac{(x - 1)\left(x - 1 + x \sqrt{9 - 16x}\right)}{1-2x}. \tag{*}$$
Now, computing the closed-form solutions of Equation ##(*)## looks like a lot of work. And even WolframAlpha returns a tremendous expression.

I'd like your help to get on with that integral.
 
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Meden Agan said:
Homework Statement: Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$
Relevant Equations: Fubini's Theorem, arcsin representation integral.

Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$

Let $$I = \int\limits_0^{\sqrt 2 / 4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx. \tag{1}$$

The representation integral of ##\arcsin## is $$\arcsin u = \int\limits_{0}^{1} \frac{\mathrm dt}{\sqrt{1-t^2}}, \qquad 0 \leqslant u \leqslant 1.$$
Plugging identity above into ##(1)## with ##u = \sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}##, we obtain
$$I = \int\limits_0^{\frac{\sqrt{2}}{4}} \frac{1}{\sqrt{x - x^2}} \int_0^{\sqrt{\frac{\left(x - 1\right) \left( x - 1 + \sqrt{9 - 16x} \right)}{1-2x}}} \frac{\mathrm dt}{\sqrt{1 - t^2}} \, \mathrm dx.$$
Since the integrand is non-negative and continuous over the rectangular domain ##D := \left\{(x, t) : 0 \leq x \leq \frac{\sqrt{2}}{4}, \,\, 0 \leq t \leq f(x)\right\}## (##f(x)## is the root of the numerator), Fubini's Theorem allows us to interchange the order:
$$I = \int\limits_0^1 \frac{\mathrm dt}{\sqrt{1 - t^2}} \int\limits_{x_*(t)}^{x^*(t)} \frac{\mathrm dx}{\sqrt{x- x^2}},$$
where ##x_*(t)## and ##x^*(t)## are the closed solutions of the equation
$$t^2 = \frac{(x - 1)\left(x - 1 + x \sqrt{9 - 16x}\right)}{1-2x}. \tag{*}$$
Now, computing the closed-form solutions of Equation ##(*)## looks like a lot of work. And even WolframAlpha returns a tremendous expression.

I'd like your help to get on with that integral.
Typo. The representation integral of ##\arcsin## is $$\arcsin u = \int\limits_{0}^{u} \frac{\mathrm dt}{\sqrt{1-t^2}}, \qquad 0 \leqslant u \leqslant 1.$$
 
I have tried to solve this by my favorite method: "remove what disturbs the most" and set ## y^2=9-16x ,## which gave me some symmetries in the integrand:
$$ \begin{align*}&\dfrac{1}{\sqrt{x-x^2}}\operatorname{arcsin}\sqrt{\dfrac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}\\
&=\sqrt{\dfrac{1}{4}-\dfrac{1}{256}(y^2-1)^2}\operatorname{arcsin}\sqrt{\dfrac{1}{32}\left(((y^2-1)+8)(y+1)-\dfrac{8}{y+1}\right)}\end{align*} $$
or
$$
\dfrac{16}{\sqrt{(8-uv)(8+uv)}}\operatorname{arcsin}\sqrt{\dfrac{(8+uv)v}{32}-\dfrac{1}{4v}}
$$
with ##u=y-1\, , \,v=y+1.## But I have no idea how to use it, or how to get rid of the single ##v## terms.

Edit: I haven't adjusted ##dx## yet, so maybe this is a chance to simplify the expression further.
 
fresh_42 said:
I have tried to solve this by my favorite method: "remove what disturbs the most" and set ## y^2=9-16x ,## which gave me some symmetries in the integrand:
$$ \begin{align*}&\dfrac{1}{\sqrt{x-x^2}}\operatorname{arcsin}\sqrt{\dfrac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}\\
&=\sqrt{\dfrac{1}{4}-\dfrac{1}{256}(y^2-1)^2}\operatorname{arcsin}\sqrt{\dfrac{1}{32}\left(((y^2-1)+8)(y+1)-\dfrac{8}{y+1}\right)}\end{align*} $$
or
$$
\dfrac{16}{\sqrt{(8-uv)(8+uv)}}\operatorname{arcsin}\sqrt{\dfrac{(8+uv)v}{32}-\dfrac{1}{4v}}
$$
with ##u=y-1\, , \,v=y+1.## But I have no idea how to use it, or how to get rid of the single ##v## terms.
Mhm... I've discovered something which puzzles me, but I have no idea how to prove it.
From post #1, we have the double integral $$I = \int\limits_0^{\frac{\sqrt{2}}{4}} \frac{1}{\sqrt{x - x^2}} \int_0^{\sqrt{\frac{\left(x - 1\right) \left( x - 1 + \sqrt{9 - 16x} \right)}{1-2x}}} \frac{\mathrm dt}{\sqrt{1 - t^2}} \, \mathrm dx.$$
If we change ##x##-bounds to ##0## and ##1## (then, ##0 \leqslant x \leqslant 1##) and ##t##-bounds to ##\frac{1}{2} \left(1- \sqrt{1-t^2}\right)## and ##\frac{1}{2} \left(1+ \sqrt{1-t^2}\right)## (then, ##\frac{1}{2} \left(1- \sqrt{1-t^2}\right) \leqslant t \leqslant \frac{1}{2} \left(1+ \sqrt{1-t^2}\right)##) we actually obtain ##\dfrac{\pi^2}{8}## as final result (interchanging order, eventually).
The integrand function must remain intact.

How do you explain this? Is it possible to perform such a change of bounds?
 
I think I have a mistake in the second line. Should probably be ##(y^2-1)^{-2}## but I haven't checked.

I don't understand your question. A better way to write an integral is ##\displaystyle{\int_{x=a}^{x=b}f(x)\,dx}## so any substitution leads to new bounds. The ##x##-bounds from ##0## to ##\sqrt{2}/4## are just nice to have all roots positive. My substitution showed me that we have only powers of ##2## everywhere, so this looks right. What do you mean by changing the bounds to ##[0,1]##? Shouldn't this result in another value? If you want that, you should substitute ##z=\dfrac{4}{\sqrt{2}} x.## I tried this first, but it didn't help a lot. Scaling is the least problem.
 
Meden Agan said:
Homework Statement: Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$
Relevant Equations: Fubini's Theorem, arcsin representation integral.

Prove $$\int\limits_0^{\sqrt2/4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx = \frac{\pi^2}{8}.$$

Let $$I = \int\limits_0^{\sqrt 2 / 4}\frac{1}{\sqrt{x-x^2}}\arcsin\sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}} \, \mathrm dx. \tag{1}$$

The representation integral of ##\arcsin## is $$\arcsin u = \int\limits_{0}^{1} \frac{\mathrm dt}{\sqrt{1-t^2}}, \qquad 0 \leqslant u \leqslant 1.$$
Plugging identity above into ##(1)## with ##u = \sqrt{\frac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}##, we obtain
$$I = \int\limits_0^{\frac{\sqrt{2}}{4}} \frac{1}{\sqrt{x - x^2}} \int_0^{\sqrt{\frac{\left(x - 1\right) \left( x - 1 + \sqrt{9 - 16x} \right)}{1-2x}}} \frac{\mathrm dt}{\sqrt{1 - t^2}} \, \mathrm dx.$$
Since the integrand is non-negative and continuous over the rectangular domain ##D := \left\{(x, t) : 0 \leq x \leq \frac{\sqrt{2}}{4}, \,\, 0 \leq t \leq f(x)\right\}## (##f(x)## is the root of the numerator), Fubini's Theorem allows us to interchange the order:
$$I = \int\limits_0^1 \frac{\mathrm dt}{\sqrt{1 - t^2}} \int\limits_{x_*(t)}^{x^*(t)} \frac{\mathrm dx}{\sqrt{x- x^2}},$$
where ##x_*(t)## and ##x^*(t)## are the closed solutions of the equation
$$t^2 = \frac{(x - 1)\left(x - 1 + x \sqrt{9 - 16x}\right)}{1-2x}. \tag{*}$$
Now, computing the closed-form solutions of Equation ##(*)## looks like a lot of work. And even WolframAlpha returns a tremendous expression.

I'd like your help to get on with that integral.
First get rid of the prefactor by going ##x=\sin^2(\theta)##, the rest should be good trigonometry.
 
pines-demon said:
First get rid of the prefactor by going ##x=\sin^2(\theta)##, the rest should be good trigonometry.
Do you mean I should substitute ##x = \sin^2 (\theta)## into ##\dfrac{(x - 1)\left(x - 1 + x \sqrt{9 - 16x}\right)}{1-2x}##? If yes, I fail to see how this helps. If not, I can't see what you mean.
 
fresh_42 said:
What do you mean by changing the bounds to ##[0,1]##? Shouldn't this result in another value?
I mean in the double integral, if we set ##t= \sqrt{\dfrac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}##, bounds of the outer integral change to ##[0,1]##. As a standard procedure for double integrals, simply substitute ##0## and ##\dfrac{\sqrt 2}{4}## into ##t= \sqrt{\dfrac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}##. Yes?
 
Let's see. We have
$$
\displaystyle{I=\int_{x=0}^{x=\sqrt{2}/4} f(x)\cdot \operatorname{arcsin} g(x) \,dx }
$$
and substitute ## g(x)=u## which I omit for clarity reasons and
$$
\operatorname{arcsin}g(x)=\int_{t=0}^{t=g(x)} \dfrac{dt}{\sqrt{1-t^2}}.
$$
This yields
\begin{align*}I&=\int_{x=0}^{x=\sqrt{2}/4} f(x)\cdot \int_{t=0}^{t=g(x)} \dfrac{dt}{\sqrt{1-t^2}} \,dx \end{align*}

Here is where it starts to become problematic. Since the inner limits depend on the outer, we cannot simply exchange the integration order. You shifted the complicated argument of the arcus sine into the upper integral limit. If you now exchange the order, then this limit hangs, so to speak, in the air.

Your solution to this mystery seems to be a rescaling of the variable ##t,## such that ##t'=g(x)=1.## But that would transfer the ugly upper bound back into the integrand. Let's see if we can rescale the other variable. Say we set ##x'=\alpha x.## Our equation now becomes
\begin{align*}
I&=\dfrac{1}{\alpha}\int_{x'=0}^{x'=\alpha\sqrt{2}/4} f\left(\dfrac{x'}{\alpha}\right)\cdot \int_{t=0}^{t=g(x'/\alpha)} \dfrac{dt}{\sqrt{1-t^2}} \,dx'
\end{align*}
and we want to choose ##\alpha## such that ##g\left(\dfrac{x'}{\alpha}\right)=1.##

This would solve your problem if you could identify the value of ##\alpha , ## but it looks awkward.

You should give @pines-demon 's idea at least a try.
 
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  • #10
fresh_42 said:
You should give @pines-demon 's idea at least a try.
I get nothing.

We have
$$I = \int_0^{\sqrt{2}/4} \frac{\arcsin\sqrt{\dfrac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}}{\sqrt{x-x^2}}\,\mathrm{d}x.$$ Under trigonometric substitution ##x=\sin^2 \theta##, with ##0 \leqslant \theta \leqslant \theta_1## and ##\theta_1 = \arcsin\sqrt{\dfrac{\sqrt{2}}{4}}##, we have ##\mathrm{d}x = 2\sin \theta \cos \theta## and ##\sqrt{x-x^2} = \sin \theta \cos \theta##. The integral becomes
$$I = 2 \int_0^{\theta_1} \arcsin \left(\sqrt{R(\theta)}\right)\,\mathrm{d}\theta, \qquad R(\theta) = \frac{\left(\sin^2\theta-1 \right)\left(\sin^2\theta-1+\sin^2\theta\sqrt{9-16\sin^2\theta}\right)}{1-2\sin^2\theta}.$$
To simplify computation, set ##A=\sin^2 \theta## and ##B=1-A=\cos^2\theta##. Then, ##\sin^2\theta-1 = -B## and ##1-2\sin^2\theta = B-A = \cos 2\theta##, while ##9-16\sin^2\theta = 1+8\cos \left(2\theta\right)##. Reassembling factors gives
$$R(\theta) = \frac{B \left(B-A\sqrt{1+8(B-A)}\right)}{B-A}.$$
Let's write ##B-A\sqrt{1+8 \left(B-A \right)}## as ##(B-A)+A \left(1-\sqrt{1+8 \, \left(B-A \right)}\right)##.
Thus:
$$\begin{aligned}
R(\theta) &= \frac{B \left[\left(B-A \right) + A \left(1-\sqrt{1+8(B-A)}\right)\right]}{B-A} \\
&= \frac{B \left(B-A \right) + AB \left(1-\sqrt{1+8(B-A)}\right)}{B-A} \\
&=\frac{B \left(B-A \right)}{\left(B-A\right)} + \frac{AB \left(1-\sqrt{1+8(B-A)}\right)}{B-A} \\
&= \frac{B \cancel{\left(B-A \right)}}{\bcancel{\left(B-A\right)}} + \frac{AB \left(1-\sqrt{1+8(B-A)}\right)}{B-A}\\
&= B + \frac{AB \left(1-\sqrt{1+8(B-A)}\right)}{B-A} \\
&= \cos^2 \theta + \frac{\sin^2 \theta \cos^2 \theta \left(1-\sqrt{1+8 \cos(2\theta)}\right)}{\cos(2 \theta)}.
\end{aligned}$$
In order for the final result to be ##\pi^2/8##, we need that ##\dfrac{\sin^2 \theta \cos^2 \theta \left(1-\sqrt{1+8 \cos(2\theta)}\right)}{\cos(2 \theta)} = 0##. And that is not true in general :-(
 
  • #11
My result is complicated, too. I wrote ##\theta=\alpha## since it is easier to type with my keyboard settings. I got for the entire integral ##I##
$$
I=2\int_0^{\operatorname{arcsin}\left(1/\sqrt[4]{8}\right)} \operatorname{arcsin}\left(
\sqrt{\dfrac{\cos^2(\alpha)-y \sin^2(\alpha)}{1-\tan^2(\alpha)}}
\right)\,d\alpha
$$
where ##y=\sqrt{(3-4\sin(\alpha))(3+4\sin(\alpha))}.##

My next step would be to use the Weierstraß substitution and see whether a polynomial expression simplifies that nasty trig expression, but I assume that we cannot get rid of the crucial term ##y.##
 
  • #12
fresh_42 said:
Let's see. We have
$$
\displaystyle{I=\int_{x=0}^{x=\sqrt{2}/4} f(x)\cdot \operatorname{arcsin} g(x) \,dx }
$$
and substitute ## g(x)=u## which I omit for clarity reasons and
$$
\operatorname{arcsin}g(x)=\int_{t=0}^{t=g(x)} \dfrac{dt}{\sqrt{1-t^2}}.
$$
This yields
\begin{align*}I&=\int_{x=0}^{x=\sqrt{2}/4} f(x)\cdot \int_{t=0}^{t=g(x)} \dfrac{dt}{\sqrt{1-t^2}} \,dx \end{align*}

Here is where it starts to become problematic. Since the inner limits depend on the outer, we cannot simply exchange the integration order. You shifted the complicated argument of the arcus sine into the upper integral limit. If you now exchange the order, then this limit hangs, so to speak, in the air.

Your solution to this mystery seems to be a rescaling of the variable ##t,## such that ##t'=g(x)=1.## But that would transfer the ugly upper bound back into the integrand. Let's see if we can rescale the other variable. Say we set ##x'=\alpha x.## Our equation now becomes
\begin{align*}
I&=\dfrac{1}{\alpha}\int_{x'=0}^{x'=\alpha\sqrt{2}/4} f\left(\dfrac{x'}{\alpha}\right)\cdot \int_{t=0}^{t=g(x'/\alpha)} \dfrac{dt}{\sqrt{1-t^2}} \,dx'
\end{align*}
and we want to choose ##\alpha## such that ##g\left(\dfrac{x'}{\alpha}\right)=1.##

This would solve your problem if you could identify the value of ##\alpha , ## but it looks awkward.
Mhm, good point.

But what I'm trying to say is something different.
I am saying I discovered that the two double integrals $$\int\limits_0^{\frac{\sqrt{2}}{4}} \frac{1}{\sqrt{x - x^2}} \int_0^{\sqrt{\frac{\left(x - 1\right) \left( x - 1 + \sqrt{9 - 16x} \right)}{1-2x}}} \frac{\mathrm dt}{\sqrt{1 - t^2}} \, \mathrm dx \tag{1}$$
and $$\int\limits_0^{1} \frac{1}{\sqrt{x - x^2}} \int_{\frac{1}{2}\left(1- \sqrt{1-t^2}\right)}^{\frac{1}{2}\left(1+ \sqrt{1-t^2}\right)} \frac{\mathrm dt}{\sqrt{1 - t^2}} \, \mathrm dx \tag{2}$$ are equivalent.

Surprisingly no change of integrand function, just a change of bounds. And evaluating the integral ##(2)## is very easy; the result is ##\dfrac{\pi^2}{8}##, as desired.

How do we explain that?
 
  • #13
How did you show equivalence without rescaling ##x## which would be necessary to change the upper bound of the outer integral? A numerical coincidence isn't proof.

And I don't understand the inner integral. How can you have the same variable in the limits as for the integration variable? This is what you should avoid by all means! Always.
 
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  • #14
fresh_42 said:
My result is complicated, too. I wrote ##\theta=\alpha## since it is easier to type with my keyboard settings. I got for the entire integral ##I##
$$
I=2\int_0^{\operatorname{arcsin}\left(1/\sqrt[4]{8}\right)} \operatorname{arcsin}\left(
\sqrt{\dfrac{\cos^2(\alpha)-y \sin^2(\alpha)}{1-\tan^2(\alpha)}}
\right)\,d\alpha
$$
where ##y=\sqrt{(3-4\sin(\alpha))(3+4\sin(\alpha))}.##

My next step would be to use the Weierstraß substitution and see whether a polynomial expression simplifies that nasty trig expression, but I assume that we cannot get rid of the crucial term ##y.##
I have no idea how to handle that...
 
  • #15
Meden Agan said:
I have no idea how to handle that...
Yes, I'm stuck, too.

We can write it as - where ##y^2=9-16x## and ##x=\sin^2(\alpha)## -
$$
I=2\int_0^{\operatorname{arcsin}(1/\sqrt[4]{8})} \operatorname{\arcsin}\left(\cos(\alpha)\sqrt{\dfrac{1-y\tan^2(\alpha)}{1-\tan^2(\alpha)}}\right)\,d\alpha
$$
I tried to set
$$
\dfrac{1-y\tan^2(\alpha)}{1-\tan^2(\alpha)}=\dfrac{\sin^2(\beta)}{\cos^2(\alpha)}
$$
but then I need the derivative according to ##\alpha## to get ##d\beta## which is a nightmare.

The expression has two difficulties: the asymmetry due to ##y=\sqrt{9-16x}## and the fact that the argument isn't a sine value, so that we can't get rid of the ##\operatorname{arcsin}.## We have a fourth root in the argument of the arcus sine and I have no idea how to handle this.

I think there is a trick for the asymmetry in ##y,## but that nasty term depends on the variable, which complicates it. The examples I have seen so far used the Taylor series of ##\operatorname{arcsin},## but that doesn't seem to be an option here. The Weierstraß substitution wasn't of help either.
 
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  • #16
I think I made a step forward. Say we abbreviate the integral by
$$
I=\int_0^{\sqrt{2}/4}\dfrac{1}{\sqrt{x-x^2}}\operatorname{arcsin}\sqrt{\dfrac{(x-1)\left(x-1+x\sqrt{9-16x}\right)}{1-2x}}\,dx
$$
and make the substitutions ##x=\sin^2(\alpha)\, , \,y^2=9-16x\, , \,a=\operatorname{arcsin}(1/\sqrt[4]{8})## and call the function
$$
f(\alpha)=\dfrac{\cos(\alpha)+\sqrt{y(\alpha)}\sin(\alpha)}{1+\tan(\alpha)}
$$
then I get a symmetric expression
$$
I=I(a)=\int_{-a}^a \operatorname{arcsin} \sqrt{f(-\alpha)f(\alpha)}\,d\alpha
$$
This is still not easy since ##f(\alpha)## is not symmetric, but at least the entire integrand and the boundaries are symmetric now. Maybe we can use this. ##f(\alpha)## alone looks like

1751202082232.webp
 
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  • #17
Relevant Equations: Fubini's Theorem, arcsin representation integral.
What is the actual statement or context of this integral? Does it explictly say that it can be calculated using Fubini's theorem? Or is this experimental math?
 
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  • #18
pines-demon said:
Does it explictly say that it can be calculated using Fubini's theorem?
No, but I just felt it was the easiest way to evaluate it.
 
  • #19
Meden Agan said:
No, but I just felt it was the easiest way to evaluate it.
So what is the context? Where you playing with numerics?
 
  • #20
pines-demon said:
So what is the context? Where you playing with numerics?
No. My instructor proposed that integral.
 
  • #21
I was worried you might all be wasting your time, but a quick numerical estimate (on Excel) indicates that the result might well be true.
 
  • #22
I gave WA the integrand, and here is what you want to calculate: the area below ...

1751202734602.webp


I also fed WA with the integral

https://www.wolframalpha.com/input?i=y(x)=integral+(from+0+to+arcsin(1/root(root(8)))+)+arcsin+(+(((cos(x)+root(root(9-16*sin^2(x)))*sin(x))/(1+tan(x)))*((cos(-x)+root(root(9-16*sin^2(-x)))*sin(-x))/(1+tan(-x))))^(1/2)+)+dx+

and I received ##I/2=0.61685## numerically versus ##\dfrac{\pi^2}{16}= 0.61685027506808491367715568749226 \ldots##

At least, I didn't make a mistake with all my substitutions and manipulations of the ##\operatorname{arcsin}## argument.

The question is really how to solve ##\displaystyle{I=\int_0^a \operatorname{arcsin}\sqrt{f(\alpha)f(-\alpha)} \,d\alpha.}##

One thing, I haven't tried so far is to use the identity
$$
\operatorname{arcsin}(xy)=-i \log\left(\sqrt{1-x^2 y^2}+ i xy\right)\,.
$$

Note: The deviation of ##\sqrt{f(\alpha)f(-\alpha)}## from a suitably scaled circle yields, with arcus sine and integral, the value ##0.636772,## only ##1\%## off.
 
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  • #23
fresh_42 said:
One thing, I haven't tried so far is to use the identity
$$
\operatorname{arcsin}(xy)=-i \log\left(\sqrt{1-x^2 y^2}+ i xy\right)\,.
$$
Mhm... Do you think that identity can make anything easier? IMO, probably complicates the integrand even more.
 
  • #24
That's why I haven't tried it so far. ##\sqrt{f(\alpha)f(-\alpha)}## looked like a perfect circle,

1751214081610.webp



but this wasn't the case, although the deviation is really small:
1751213882558.webp


This nasty little bulk makes the function so complicated. Our curve is a circle with a flat spot around ##1/2.##

I'm currently back at
$$
f(\alpha)f(-\alpha)=\dfrac{1}{32}\dfrac{(y^2+7)(y^2+2y-7)}{y+1}
$$
and look for a parameterization that is suited to draw the root and apply the arcus sine. The fact that the result can be noted exactly is the curse here. It makes you think that there is a hidden trick somewhere.
 
  • #25
Meden Agan said:
No. My instructor proposed that integral.
Is an instructor for an undergrad course? is the integral physics related? Is it a course of math, physics or something in particular? what techniques would they expect you to know? Any additional context would help
 
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  • #27
renormalize said:
It turns out that this very integral was posted 5 days ago on Mathematics Stack Exchange by "Dan" (is that you @Meden Agan ?): https://math.stackexchange.com/ques...4-frac1-sqrtx-x2-arcsin-sqrt-fracx-1x-1x-sqrt
The first answer there by "user170231" provides an impressive proof in terms of dilogarithms.
Mhm... A delightful surprise! Most likely my instructor took that integral from there.
However, I would be interested to hear what we get with @fresh_42's method in post #24 :-)
 
  • #28
fresh_42 said:
The question is really how to solve ##\displaystyle{I=\int_0^a \operatorname{arcsin}\sqrt{f(\alpha)f(-\alpha)} \,d\alpha.}##
How about differentiation under integral sign or integral representation of ##\arcsin##? What do you think?
 
  • #29
Meden Agan said:
How about differentiation under integral sign or integral representation of ##\arcsin##? What do you think?
I think that there are nice possibilities to get rid of the arcus sine.

I used
\begin{align*}
I&=2\int_{0}^a \operatorname{arcsin} \sqrt{f(\alpha)f(-\alpha)}\,d\alpha=2\int_{0}^a\int_0^1 \sqrt{\dfrac{f(\alpha)f(-\alpha)}{1-f(\alpha)f(-\alpha)t^2}}\,dt\,d\alpha \\
&=2\int_{0}^a\int_0^1 \dfrac{1}{\sqrt{\left(f(\alpha)f(-\alpha)\right)^{-1}-t^2}}\,dt\,d\alpha\\
&=2\int_{0}^a\int_0^1\dfrac{1}{\sqrt{\dfrac{32(y+1)}{(y^2+2y-7)(y^2+7)}-t^2}}\,dt\,d\alpha
\end{align*}
where ##a=\operatorname{arcsin}(1/\sqrt{8})\, , \,y^2=9-16 x\, , \,x=\sin^2(\alpha)## and
$$
f(\alpha)f(-\alpha)=\dfrac{1}{32}\dfrac{(y^2+2y-7)(y^2+7)}{y+1}
$$
However, Fubini or not, it leads me directly into the same complicated - now polynomial - integrations as dealt with on MSE.

I have found another funny formula on Wikipedia that at least provide the additional ##\pi## and the logarithm which is apparently part of the deal:
$$
\operatorname{arcsin}R(x) = \int_0^1 \dfrac{1}{\pi \,t}\log\left(\dfrac{t^2+2R(x)t+1}{t^2-2R(x)t+1}\right) \;dt
$$

Looking at the math on MSE shows that there is no easy way to deal with the integrations, even without the trig function.
 
  • #30
fresh_42 said:
I think that there are nice possibilities to get rid of the arcus sine.

I used
\begin{align*}
I&=2\int_{0}^a \operatorname{arcsin} \sqrt{f(\alpha)f(-\alpha)}\,d\alpha=2\int_{0}^a\int_0^1 \sqrt{\dfrac{f(\alpha)f(-\alpha)}{1-f(\alpha)f(-\alpha)t^2}}\,dt\,d\alpha \\
&=2\int_{0}^a\int_0^1 \dfrac{1}{\sqrt{\left(f(\alpha)f(-\alpha)\right)^{-1}-t^2}}\,dt\,d\alpha\\
&=2\int_{0}^a\int_0^1\dfrac{1}{\sqrt{\dfrac{32(y+1)}{(y^2+2y-7)(y^2+7)}-t^2}}\,dt\,d\alpha
\end{align*}
where ##a=\operatorname{arcsin}(1/\sqrt{8})\, , \,y^2=9-16 x\, , \,x=\sin^2(\alpha)## and
$$
f(\alpha)f(-\alpha)=\dfrac{1}{32}\dfrac{(y^2+2y-7)(y^2+7)}{y+1}
$$
However, Fubini or not, it leads me directly into the same complicated - now polynomial - integrations as dealt with on MSE.
This whole thing is frankly unmanageable. Perhaps changing the upper bound to the inner integral (by giving it as a function of ##\alpha##)? I mean, maybe a different integral representation of ##\arcsin##.
What do you think?
 

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