r=1∑∞n4+r4n−(n2+r2)n4+r42nr2r=1∑∞1+(nr)4n1−(1+(nr)2)1+(nr)42(n1)(nr)2⇒∫011+x4dx−(1+x2)1+x42x2dx⇒∫01(1+x2)1+x41−x2dx⇒∫01(x+x1)x2+x21x21−1dx ⇒−∫01(x+x1)(x+x1)2−21−x21dxx+x1=t⇒1−x21dx=dt ⇒−∫∞2tt2−2dt⇒−∫∞2t2t2−2tdt take t2−2=α2tdt=αdα⇒−∫∞2(α2+2)ααdα⇒−∫∞2α2+2dα $\begin{aligned}
& \left.\Rightarrow \frac{-1}{\sqrt{2}} \tan ^{-1} \frac{\alpha}{\sqrt{2}}\right]_{\infty}^{\sqrt{2}} \
& \Rightarrow \frac{-1}{\sqrt{2}}\left{\tan ^{-1} 1\right}+\frac{1}{\sqrt{2}} \tan ^{-1} \infty \
& \Rightarrow \frac{1}{\sqrt{2}}\left{\frac{\pi}{2}-\frac{\pi}{4}\right} \
& \Rightarrow \frac{\pi}{4 \sqrt{2}}=\frac{\pi}{\mathrm{K}}
\end{aligned}$
So K=42 K2=32