arildno said:
Not utterly trivial, Rainbow Child:
Although the "radial" integration will go easy enough, the limits for the unit square, as represented in polar coordinates are somewhat nasty.
You are right, this
Rainbow Child said:
was stupid statement, since I didn't paid much attention to the limits of the integration. Even though the resulting can be evaluted without by hand (but not trivially

!).
The region of integration in polar coordinates becames
[tex]\mathcal{D}_1=\left\{(r,\theta):0<\theta<\frac{\pi}{4},0<r<\frac{1}{\cos\theta}\right\},\, \mathcal{D}_2=\left\{(r,\theta):\frac{\pi}{4}<\theta<\frac{\pi}{2},0<r<\frac{1}{\sin\theta}\right\}[/tex]
thus
[tex]I=\int_0^1 \int_0^1 dx dy \frac{1}{(1+x^2+y^2)^{5/2}}=\int\int_{\mathcal{D}_1}d\theta\,dr\frac{r}{(1+r^2)^{5/2}}+\int\int_{\mathcal{D}_2}d\theta\,dr\frac{r}{(1+r^2)^{5/2}}=I_1+I_2[/tex]
The first integral [tex]I_1[/tex] reads
[tex]I_1=\int_0^{\frac{\pi}{4}}d\theta\int_0^{1/\cos\theta}dr\frac{r}{(1+r^2)^{5/2}}=-\frac{1}{3}\int_0^{\frac{\pi}{4}}d\theta\left(\frac{1}{(1+1/\cos^2\theta)^{3/2}}-1\right)=-\frac{1}{3}\int_0^{\frac{\pi}{4}}d\theta\frac{\cos^3\theta}{(1+\cos^2\theta)^{3/2}}+\frac{\pi}{12}=-\frac{1}{3}\,J_1+\frac{\pi}{12}[/tex]
The integral [tex]J_1[/tex] reads
[tex]J_1=\int_0^{\frac{\sqrt{2}}{2}}d(\sin\theta)\frac{\cos^2\theta}{(1+\cos^2\theta)^{3/2}}=\int_0^{\frac{\sqrt{2}}{2}}d(\sin\theta)\frac{1-\sin^2\theta}{(2-\sin^2\theta)^{3/2}}}}=\int_0^{\frac{\sqrt{2}}{2}}dt\frac{2-t^2}{(2-t^2)^{3/2}}-\int_0^{\frac{\sqrt{2}}{2}}dt\frac{1}{(2-t^2)^{3/2}}=\arcsin\frac{t}{\sqrt{2}}\Big|_0^{\frac{\sqrt{2}}{2}}-\frac{t}{2\,\sqrt{2-t^2}}\Big|_0^{\frac{\sqrt{2}}{2}}\Rightarrow[/tex]
[tex]J_1=\frac{\pi}{6}-\frac{\sqrt{3}}{6}\Rightarrow I_1=\frac{\sqrt{3}}{18}+\frac{\pi}{36}[/tex]
Similary for the 2nd integral [tex]I_2[/tex] we have
[tex]I_2=\frac{\sqrt{3}}{18}+\frac{\pi}{36}[/tex]
yielding to
[tex]I=\frac{\pi}{18}+\frac{\sqrt{3}}{9}[/tex]
as coomast and Troels posted.
Obviously not trivial!
