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Question Number 63395 by mathmax by abdo last updated on 03/Jul/19

let f(t) =∫_0 ^∞  ((ln(1+tx))/(1+x^2 ))dx   with  ∣t∣<1  1) determine a explicit  form of f(t)  2) find the value of ∫_0 ^∞    ((ln(1+x))/(1+x^2 ))dx

$${let}\:{f}\left({t}\right)\:=\int_{\mathrm{0}} ^{\infty} \:\frac{{ln}\left(\mathrm{1}+{tx}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:\:\:{with}\:\:\mid{t}\mid<\mathrm{1} \\ $$ $$\left.\mathrm{1}\right)\:{determine}\:{a}\:{explicit}\:\:{form}\:{of}\:{f}\left({t}\right) \\ $$ $$\left.\mathrm{2}\right)\:{find}\:{the}\:{value}\:{of}\:\int_{\mathrm{0}} ^{\infty} \:\:\:\frac{{ln}\left(\mathrm{1}+{x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx} \\ $$

Commented byPrithwish sen last updated on 03/Jul/19

f(t)=∫_0 ^∞ ((ln(1+tx))/(1+x^2 )) dt  f′(t) = ∫_0 ^∞ (δ/(δt)){((ln(1+tx))/(1+x^2 )) }dx           = ∫_0 ^∞ (x/((1+x^2 )(1+tx))) dx         = (1/(1+t^2 )) ∫_0 ^B {(x/(1+x^2 )) +(t/(1+x^2 )) −(t/(1+tx)) }dx, B→∞        = (1/(1+t^2 )) [ ln(((√(1+x^2 ))/(1+tx))) + t( tan^(−1) x)]_0 ^B   B→∞     Now, lim_(B→∞)  ln (((√(1+x^2 ))/(1+tx))) ⇒ lim_(B→∞) ln(((√(1+B^2 ))/(1+Bt)))  put B= (1/n) ⇒ lim_(n→0)  ln(((√(n^2 +1))/(n+t)))⇒ −ln(t)   ∴  f(t) = −∫((ln(t))/(1+t^2 )) dt+ (π/2) ∫((tdt)/(1+t^(2 ) ))  to be continue.......

$$\mathrm{f}\left(\mathrm{t}\right)=\int_{\mathrm{0}} ^{\infty} \frac{\mathrm{ln}\left(\mathrm{1}+\mathrm{tx}\right)}{\mathrm{1}+\mathrm{x}^{\mathrm{2}} }\:\mathrm{dt} \\ $$ $$\mathrm{f}'\left(\mathrm{t}\right)\:=\:\int_{\mathrm{0}} ^{\infty} \frac{\delta}{\delta\mathrm{t}}\left\{\frac{\mathrm{ln}\left(\mathrm{1}+\mathrm{tx}\right)}{\mathrm{1}+\mathrm{x}^{\mathrm{2}} }\:\right\}\mathrm{dx} \\ $$ $$\:\:\:\:\:\:\:\:\:=\:\int_{\mathrm{0}} ^{\infty} \frac{\mathrm{x}}{\left(\mathrm{1}+\mathrm{x}^{\mathrm{2}} \right)\left(\mathrm{1}+\mathrm{tx}\right)}\:\mathrm{dx} \\ $$ $$\:\:\:\:\:\:\:=\:\frac{\mathrm{1}}{\mathrm{1}+\mathrm{t}^{\mathrm{2}} }\:\int_{\mathrm{0}} ^{\mathrm{B}} \left\{\frac{\mathrm{x}}{\mathrm{1}+\mathrm{x}^{\mathrm{2}} }\:+\frac{\mathrm{t}}{\mathrm{1}+\mathrm{x}^{\mathrm{2}} }\:−\frac{\mathrm{t}}{\mathrm{1}+\mathrm{tx}}\:\right\}\mathrm{dx},\:\mathrm{B}\rightarrow\infty \\ $$ $$\:\:\:\:\:\:=\:\frac{\mathrm{1}}{\mathrm{1}+\mathrm{t}^{\mathrm{2}} }\:\left[\:\mathrm{ln}\left(\frac{\sqrt{\mathrm{1}+\mathrm{x}^{\mathrm{2}} }}{\mathrm{1}+\mathrm{tx}}\right)\:+\:\mathrm{t}\left(\:\mathrm{tan}^{−\mathrm{1}} \mathrm{x}\right)\right]_{\mathrm{0}} ^{\mathrm{B}} \:\:\mathrm{B}\rightarrow\infty \\ $$ $$\:\:\:\mathrm{Now},\:\mathrm{lim}_{\mathrm{B}\rightarrow\infty} \:\mathrm{ln}\:\left(\frac{\sqrt{\mathrm{1}+\mathrm{x}^{\mathrm{2}} }}{\mathrm{1}+\mathrm{tx}}\right)\:\Rightarrow\:\mathrm{lim}_{\mathrm{B}\rightarrow\infty} \mathrm{ln}\left(\frac{\sqrt{\mathrm{1}+\mathrm{B}^{\mathrm{2}} }}{\mathrm{1}+\mathrm{Bt}}\right) \\ $$ $$\mathrm{put}\:\mathrm{B}=\:\frac{\mathrm{1}}{\mathrm{n}}\:\Rightarrow\:\mathrm{lim}_{\mathrm{n}\rightarrow\mathrm{0}} \:\mathrm{ln}\left(\frac{\sqrt{\mathrm{n}^{\mathrm{2}} +\mathrm{1}}}{\mathrm{n}+\mathrm{t}}\right)\Rightarrow\:−\mathrm{ln}\left(\mathrm{t}\right) \\ $$ $$\:\therefore\:\:\mathrm{f}\left(\mathrm{t}\right)\:=\:−\int\frac{\mathrm{ln}\left(\mathrm{t}\right)}{\mathrm{1}+\mathrm{t}^{\mathrm{2}} }\:\mathrm{dt}+\:\frac{\pi}{\mathrm{2}}\:\int\frac{\mathrm{tdt}}{\mathrm{1}+\mathrm{t}^{\mathrm{2}\:} } \\ $$ $$\mathrm{to}\:\mathrm{be}\:\mathrm{continue}....... \\ $$ $$ \\ $$

Commented bymathmax by abdo last updated on 04/Jul/19

1) we have f^′ (t) =∫_0 ^∞   (x/((x^2 +1)(1+tx)))dx  let decompose F(x)=(x/((tx+1)(x^2  +1)))  F(x)=(a/(tx+1)) +((bx+c)/(x^2  +1))  a=lim_(x→−(1/t))    (tx+1)F(x)=((−1)/(t((1/t^2 )+1))) =((−t^2 )/(t(1+t^2 ))) =−(t/(1+t^2 ))  lim_(x→+∞) xF(x)=0=(a/t) +b ⇒b=−(a/t) =(1/(1+t^2 )) ⇒F(x)=−(t/((1+t^2 )(tx+1))) +(((x/(1+t^2 ))+c)/(x^2  +1))  F(0)=0 =−(t/(1+t^2 )) +c ⇒c =(t/(1+t^2 )) ⇒  F(x)=((−t)/((1+t^2 )(tx+1))) +(1/(1+t^2 )) ((x+t)/(x^2  +1)) ⇒  f^′ (t) =((−t)/(1+t^2 )) ∫_0 ^∞    (dx/(tx+1)) +(1/(2(1+t^2 ))) ∫_0 ^∞    ((2x)/(x^2  +1))dx +(t/(1+t^2 ))∫_0 ^∞   (dx/(1+x^2 ))  =(1/(1+t^2 )){ [(1/2)ln(x^2 +1)−ln∣tx +1∣]_0 ^(+∞) } +((πt)/(2(1+t^2 )))  =(1/(1+t^2 ))[ln∣((√(x^2 +1))/(tx+1))∣]_0 ^(+∞)  +((πt)/(2(1+t^2 ))) =(1/(1+t^2 ))ln((1/t^2 )) +((πt)/(2(1+t^2 )))  =−((ln∣t∣)/(1+t^2 )) +((πt)/(2(1+t^2 ))) ⇒  f(t) =−∫_0 ^t   ((lnx)/(1+x^2 ))dx  +(π/2) ∫_0 ^t   (x/(1+x^2 )) dx +C  =−∫_0 ^t    ((lnx)/(1+x^2 ))dx +(π/4)ln(1+t^2 ) +C  C=f(0) =0 ⇒f(t) = (π/4)ln(1+t^2 )−∫_0 ^t   ((lnx)/(1+x^2 ))dx     (we suppose t≥0)  2) we have ∫_0 ^∞    ((ln(1+x))/(1+x^2 ))dx =f(1) =(π/4)ln(2)−∫_0 ^1  ((ln(x))/(1+x^2 ))dx  changement  x =tanθ give    ((ln(x))/(1+x^2 ))dx = ∫_0 ^(π/4)   ((ln(tanθ))/(1+tan^2 θ))(1+tan^2 θ)dθ = ∫_0 ^(π/4)  ln(tanθ)dθ  =[θ ln(tanθ) ]_0 ^(π/4)  −∫_0 ^(π/4)   θ ((1+tan^2 θ)/(tanθ)) dθ =−∫_0 ^(π/4)   θ  (1/(cos^2 θ ((sinθ)/(cosθ))))dθ  =∫_0 ^(π/4)     (θ/(cosθ sinθ)) dθ = 2 ∫_0 ^(π/4)    (θ/(sin(2θ)))dθ =_(2θ =u)    2 ∫_0 ^(π/2)   (u/(2sin(u))) (du/2)  =(1/2) ∫_0 ^(π/2)    (u/(sinu)) du =_(tan((u/2))=α)    (1/2) ∫_0 ^1    ((2arctan(α))/((2α)/(1+α^2 ))) ((2dα)/(1+α^2 ))  =(1/2) ∫_0 ^1    ((arctan(α))/α) dα     ...be continued...

$$\left.\mathrm{1}\right)\:{we}\:{have}\:{f}^{'} \left({t}\right)\:=\int_{\mathrm{0}} ^{\infty} \:\:\frac{{x}}{\left({x}^{\mathrm{2}} +\mathrm{1}\right)\left(\mathrm{1}+{tx}\right)}{dx}\:\:{let}\:{decompose}\:{F}\left({x}\right)=\frac{{x}}{\left({tx}+\mathrm{1}\right)\left({x}^{\mathrm{2}} \:+\mathrm{1}\right)} \\ $$ $${F}\left({x}\right)=\frac{{a}}{{tx}+\mathrm{1}}\:+\frac{{bx}+{c}}{{x}^{\mathrm{2}} \:+\mathrm{1}} \\ $$ $${a}={lim}_{{x}\rightarrow−\frac{\mathrm{1}}{{t}}} \:\:\:\left({tx}+\mathrm{1}\right){F}\left({x}\right)=\frac{−\mathrm{1}}{{t}\left(\frac{\mathrm{1}}{{t}^{\mathrm{2}} }+\mathrm{1}\right)}\:=\frac{−{t}^{\mathrm{2}} }{{t}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)}\:=−\frac{{t}}{\mathrm{1}+{t}^{\mathrm{2}} } \\ $$ $${lim}_{{x}\rightarrow+\infty} {xF}\left({x}\right)=\mathrm{0}=\frac{{a}}{{t}}\:+{b}\:\Rightarrow{b}=−\frac{{a}}{{t}}\:=\frac{\mathrm{1}}{\mathrm{1}+{t}^{\mathrm{2}} }\:\Rightarrow{F}\left({x}\right)=−\frac{{t}}{\left(\mathrm{1}+{t}^{\mathrm{2}} \right)\left({tx}+\mathrm{1}\right)}\:+\frac{\frac{{x}}{\mathrm{1}+{t}^{\mathrm{2}} }+{c}}{{x}^{\mathrm{2}} \:+\mathrm{1}} \\ $$ $${F}\left(\mathrm{0}\right)=\mathrm{0}\:=−\frac{{t}}{\mathrm{1}+{t}^{\mathrm{2}} }\:+{c}\:\Rightarrow{c}\:=\frac{{t}}{\mathrm{1}+{t}^{\mathrm{2}} }\:\Rightarrow \\ $$ $${F}\left({x}\right)=\frac{−{t}}{\left(\mathrm{1}+{t}^{\mathrm{2}} \right)\left({tx}+\mathrm{1}\right)}\:+\frac{\mathrm{1}}{\mathrm{1}+{t}^{\mathrm{2}} }\:\frac{{x}+{t}}{{x}^{\mathrm{2}} \:+\mathrm{1}}\:\Rightarrow \\ $$ $${f}^{'} \left({t}\right)\:=\frac{−{t}}{\mathrm{1}+{t}^{\mathrm{2}} }\:\int_{\mathrm{0}} ^{\infty} \:\:\:\frac{{dx}}{{tx}+\mathrm{1}}\:+\frac{\mathrm{1}}{\mathrm{2}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)}\:\int_{\mathrm{0}} ^{\infty} \:\:\:\frac{\mathrm{2}{x}}{{x}^{\mathrm{2}} \:+\mathrm{1}}{dx}\:+\frac{{t}}{\mathrm{1}+{t}^{\mathrm{2}} }\int_{\mathrm{0}} ^{\infty} \:\:\frac{{dx}}{\mathrm{1}+{x}^{\mathrm{2}} } \\ $$ $$=\frac{\mathrm{1}}{\mathrm{1}+{t}^{\mathrm{2}} }\left\{\:\left[\frac{\mathrm{1}}{\mathrm{2}}{ln}\left({x}^{\mathrm{2}} +\mathrm{1}\right)−{ln}\mid{tx}\:+\mathrm{1}\mid\right]_{\mathrm{0}} ^{+\infty} \right\}\:+\frac{\pi{t}}{\mathrm{2}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)} \\ $$ $$=\frac{\mathrm{1}}{\mathrm{1}+{t}^{\mathrm{2}} }\left[{ln}\mid\frac{\sqrt{{x}^{\mathrm{2}} +\mathrm{1}}}{{tx}+\mathrm{1}}\mid\right]_{\mathrm{0}} ^{+\infty} \:+\frac{\pi{t}}{\mathrm{2}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)}\:=\frac{\mathrm{1}}{\mathrm{1}+{t}^{\mathrm{2}} }{ln}\left(\frac{\mathrm{1}}{{t}^{\mathrm{2}} }\right)\:+\frac{\pi{t}}{\mathrm{2}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)} \\ $$ $$=−\frac{{ln}\mid{t}\mid}{\mathrm{1}+{t}^{\mathrm{2}} }\:+\frac{\pi{t}}{\mathrm{2}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)}\:\Rightarrow \\ $$ $${f}\left({t}\right)\:=−\int_{\mathrm{0}} ^{{t}} \:\:\frac{{lnx}}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:\:+\frac{\pi}{\mathrm{2}}\:\int_{\mathrm{0}} ^{{t}} \:\:\frac{{x}}{\mathrm{1}+{x}^{\mathrm{2}} }\:{dx}\:+{C} \\ $$ $$=−\int_{\mathrm{0}} ^{{t}} \:\:\:\frac{{lnx}}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:+\frac{\pi}{\mathrm{4}}{ln}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)\:+{C} \\ $$ $${C}={f}\left(\mathrm{0}\right)\:=\mathrm{0}\:\Rightarrow{f}\left({t}\right)\:=\:\frac{\pi}{\mathrm{4}}{ln}\left(\mathrm{1}+{t}^{\mathrm{2}} \right)−\int_{\mathrm{0}} ^{{t}} \:\:\frac{{lnx}}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:\:\:\:\:\left({we}\:{suppose}\:{t}\geqslant\mathrm{0}\right) \\ $$ $$\left.\mathrm{2}\right)\:{we}\:{have}\:\int_{\mathrm{0}} ^{\infty} \:\:\:\frac{{ln}\left(\mathrm{1}+{x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:={f}\left(\mathrm{1}\right)\:=\frac{\pi}{\mathrm{4}}{ln}\left(\mathrm{2}\right)−\int_{\mathrm{0}} ^{\mathrm{1}} \:\frac{{ln}\left({x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx} \\ $$ $${changement}\:\:{x}\:={tan}\theta\:{give}\: \\ $$ $$\:\frac{{ln}\left({x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:=\:\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{4}}} \:\:\frac{{ln}\left({tan}\theta\right)}{\mathrm{1}+{tan}^{\mathrm{2}} \theta}\left(\mathrm{1}+{tan}^{\mathrm{2}} \theta\right){d}\theta\:=\:\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{4}}} \:{ln}\left({tan}\theta\right){d}\theta \\ $$ $$=\left[\theta\:{ln}\left({tan}\theta\right)\:\right]_{\mathrm{0}} ^{\frac{\pi}{\mathrm{4}}} \:−\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{4}}} \:\:\theta\:\frac{\mathrm{1}+{tan}^{\mathrm{2}} \theta}{{tan}\theta}\:{d}\theta\:=−\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{4}}} \:\:\theta\:\:\frac{\mathrm{1}}{{cos}^{\mathrm{2}} \theta\:\frac{{sin}\theta}{{cos}\theta}}{d}\theta \\ $$ $$=\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{4}}} \:\:\:\:\frac{\theta}{{cos}\theta\:{sin}\theta}\:{d}\theta\:=\:\mathrm{2}\:\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{4}}} \:\:\:\frac{\theta}{{sin}\left(\mathrm{2}\theta\right)}{d}\theta\:=_{\mathrm{2}\theta\:={u}} \:\:\:\mathrm{2}\:\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{2}}} \:\:\frac{{u}}{\mathrm{2}{sin}\left({u}\right)}\:\frac{{du}}{\mathrm{2}} \\ $$ $$=\frac{\mathrm{1}}{\mathrm{2}}\:\int_{\mathrm{0}} ^{\frac{\pi}{\mathrm{2}}} \:\:\:\frac{{u}}{{sinu}}\:{du}\:=_{{tan}\left(\frac{{u}}{\mathrm{2}}\right)=\alpha} \:\:\:\frac{\mathrm{1}}{\mathrm{2}}\:\int_{\mathrm{0}} ^{\mathrm{1}} \:\:\:\frac{\mathrm{2}{arctan}\left(\alpha\right)}{\frac{\mathrm{2}\alpha}{\mathrm{1}+\alpha^{\mathrm{2}} }}\:\frac{\mathrm{2}{d}\alpha}{\mathrm{1}+\alpha^{\mathrm{2}} } \\ $$ $$=\frac{\mathrm{1}}{\mathrm{2}}\:\int_{\mathrm{0}} ^{\mathrm{1}} \:\:\:\frac{{arctan}\left(\alpha\right)}{\alpha}\:{d}\alpha\:\:\:\:\:...{be}\:{continued}... \\ $$

Commented bymathmax by abdo last updated on 04/Jul/19

let try another way we have ∫_0 ^∞   ((ln(1+x))/(1+x^2 ))dx =(π/4)ln(2)−∫_0 ^1  ((ln(x))/(1+x^2 ))dx  ∫_0 ^1  ((ln(x))/(1+x^2 ))dx =∫_0 ^1 ln(x)(Σ_(n=0) ^∞  (−1)^n  x^(2n) )dx  =Σ_(n=0) ^∞ (−1)^n  ∫_0 ^1  x^(2n) ln(x)dx  by[parts  ∫_0 ^1   x^(2n) ln(x)dx =[(1/(2n+1))x^(2n+1) ln(x)]_0 ^1  −∫_0 ^1  (1/(2n+1))x^(2n+1)  (dx/x)  =−(1/(2n+1)) ∫_0 ^1  x^(2n) dx =−(1/((2n+1)^2 )) ⇒∫_0 ^1   ((ln(x))/(1+x^2 ))dx =−Σ_(n=0) ^∞  (((−1)^n )/((2n+1)^2 ))  rest to find the value of this serie   by fourier series.....

$${let}\:{try}\:{another}\:{way}\:{we}\:{have}\:\int_{\mathrm{0}} ^{\infty} \:\:\frac{{ln}\left(\mathrm{1}+{x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:=\frac{\pi}{\mathrm{4}}{ln}\left(\mathrm{2}\right)−\int_{\mathrm{0}} ^{\mathrm{1}} \:\frac{{ln}\left({x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx} \\ $$ $$\int_{\mathrm{0}} ^{\mathrm{1}} \:\frac{{ln}\left({x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:=\int_{\mathrm{0}} ^{\mathrm{1}} {ln}\left({x}\right)\left(\sum_{{n}=\mathrm{0}} ^{\infty} \:\left(−\mathrm{1}\right)^{{n}} \:{x}^{\mathrm{2}{n}} \right){dx} \\ $$ $$=\sum_{{n}=\mathrm{0}} ^{\infty} \left(−\mathrm{1}\right)^{{n}} \:\int_{\mathrm{0}} ^{\mathrm{1}} \:{x}^{\mathrm{2}{n}} {ln}\left({x}\right){dx}\:\:{by}\left[{parts}\right. \\ $$ $$\int_{\mathrm{0}} ^{\mathrm{1}} \:\:{x}^{\mathrm{2}{n}} {ln}\left({x}\right){dx}\:=\left[\frac{\mathrm{1}}{\mathrm{2}{n}+\mathrm{1}}{x}^{\mathrm{2}{n}+\mathrm{1}} {ln}\left({x}\right)\right]_{\mathrm{0}} ^{\mathrm{1}} \:−\int_{\mathrm{0}} ^{\mathrm{1}} \:\frac{\mathrm{1}}{\mathrm{2}{n}+\mathrm{1}}{x}^{\mathrm{2}{n}+\mathrm{1}} \:\frac{{dx}}{{x}} \\ $$ $$=−\frac{\mathrm{1}}{\mathrm{2}{n}+\mathrm{1}}\:\int_{\mathrm{0}} ^{\mathrm{1}} \:{x}^{\mathrm{2}{n}} {dx}\:=−\frac{\mathrm{1}}{\left(\mathrm{2}{n}+\mathrm{1}\right)^{\mathrm{2}} }\:\Rightarrow\int_{\mathrm{0}} ^{\mathrm{1}} \:\:\frac{{ln}\left({x}\right)}{\mathrm{1}+{x}^{\mathrm{2}} }{dx}\:=−\sum_{{n}=\mathrm{0}} ^{\infty} \:\frac{\left(−\mathrm{1}\right)^{{n}} }{\left(\mathrm{2}{n}+\mathrm{1}\right)^{\mathrm{2}} } \\ $$ $${rest}\:{to}\:{find}\:{the}\:{value}\:{of}\:{this}\:{serie}\:\:\:{by}\:{fourier}\:{series}..... \\ $$

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