Find the sum of$$\sum _{r=1}^\infty\left({\frac{2}{4r-3}-\frac{1}{2r}}\right)$$ I tried to solve this problem by taking $2$ common from the expression and got the result as of$$2\sum _{r=1}^\infty\left({\frac{1}{4r-3}-\frac{1}{4r}}\right)$$ but I could not get any constant term on which I could apply the telescopic series formula please help me out.
A Question based on series.
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$$S_n=\sum _{r=1}^n \left(\frac{2}{4r-3}-\frac{1}{2r}\right)=\frac12\sum _{r=1}^n \left(\frac{1}{r+\frac14-1}-\frac{1}{r+1-1}\right)$$ It is a easy problem to people familiar with the polygamma functions. $$\sum _{r=1}^n \frac{1}{r+a-1}=\psi(a+n)-\psi(a)$$ $\psi(x)$ is the digamma function.
Successively with $a=\frac14$ and $a=1$ : $$S_n=\frac12\left(\psi\left(\frac14+n\right)-\psi\left(\frac14\right)-\psi\left(1+n\right)+\psi\left(1\right)\right)$$ $n\to\infty\quad \psi(a+n)\sim \ln(n)+O\left(\frac{1}{x}\right)$
$\lim_{n\to\infty}\left(\psi\left(\frac14+n\right)-\psi\left(1+n\right)\right)=0$ $$S_\infty=\frac12\left(-\psi\left(-\frac14\right)+\psi\left(1\right)\right)$$ $\psi(1)=-\gamma$ Euler-Mascheroni constant. And $\psi(1/4)=-\gamma-\frac{\pi}{2}-3\ln(2)$ $$S_\infty=\frac12\left(\frac{\pi}{2}+3\ln(2)\right)$$ $$\sum _{r=1}^\infty \left(\frac{2}{4r-3}-\frac{1}{2r}\right)=\frac{\pi}{4}+\frac32\ln(2)$$ For reference : http://mathworld.wolfram.com/DigammaFunction.html
This is not a telescopic series, though it might superficially resemble one.
The common technique with such problems is to transform them to power series (by putting $x^n$ or something in the numerator), then fiddle around with functions, their Taylor series, maybe some differentiation or other stuff, and then evaluate the series at $x=1$.
Short of that, we are reduced to using the following crude tools.
Suppose you know that $\sum\limits_{n=1}^\infty{(-1)^{n+1}\over n}=\ln2$ (because if you don't, we aren't going anywhere). Suppose you also know that $\sum\limits_{n=1}^\infty{(-1)^{n+1}\over 2n+1}={\pi\over4}$, which is also a mandatory prerequisite. Then, obviously $$\sum_{n=1}^\infty{(-1)^{n+1}\over 2n}={1\over2}\sum_{n=1}^\infty{(-1)^{n+1}\over n}={\ln2\over2}$$ Now I'm going to put it in a simple way, without all those fancy $\sum$s: $$\begin{array}{ccccccccccc} {\pi\over4} &=& 1 & & -{1\over3} & & +{1\over5} & & -{1\over7} &\dots \\ \ln 2 &=& 1 & -{1\over2} & +{1\over3} & -{1\over4} & +{1\over5} & -{1\over6} & +{1\over7} &\dots \\ {\ln 2\over2} &=& & \phantom{-}{1\over2} & & -{1\over4} & & +{1\over6} & &\dots \\ \end{array}$$ Now just add these three series together.