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Question Number 119462 by mnjuly1970 last updated on 24/Oct/20

          ... advanced calculus...       evaluate ::                           Ω=∫_0 ^( ∞)  ((tan^(−1) (x))/(e^(2πx) −1))dx =?                    m.n.1970

...advancedcalculus...evaluate::Ω=0tan1(x)e2πx1dx=?m.n.1970

Answered by mathmax by abdo last updated on 25/Oct/20

let take a try with series  A =∫_0 ^∞  ((arctanx)/(e^(2πx) −1))dx ⇒A =∫_0 ^∞   ((e^(−2πx) arctanx)/(1−e^(−2πx) ))dx  =∫_0 ^∞  e^(−2πx) arctanxΣ_(n=0) ^∞ e^(−2nπx) dx  =Σ_(n=0) ^∞  ∫_0 ^∞  e^(−2π(n+1)x)  arctanx dx =Σ_(n=0) ^∞ A_n   A_n =∫_0 ^∞  e^(−2π(n+1)x) arctanx dx  =_(by parts)    [−(e^(−2π(n+1)x) /(2π(n+1))) arctanx]_0 ^∞ +∫_0 ^∞  (e^(−2π(n+1)x) /(2π(n+1)))×(dx/(1+x^2 ))  =(1/(2π(n+1)))∫_0 ^∞  (e^(−2π(n+1)x) /(1+x^2 ))dx =_(2π(n+1)x=t) (1/(2π(n+1)))∫_0 ^∞  (e^(−t) /(1+(t^2 /(4π^2 (n+1)^2 ))))×(dt/(2π(n+1)))  =(1/(4π^2 (n+1)^2 )) ∫_0 ^∞   (e^(−t) /(t^2 +4π^2 (n+1)^2 ))×4π^2 (n+1)^2 dt  =∫_0 ^∞   (e^(−t) /(t^2 +4π^2 (n+1)^2 ))dt =∫_0 ^∞ (1/(t^2 +4π^2 (n+1)^2 ))(Σ_(p=0) ^∞  (((−t)^p )/(p!)))dt  =Σ_(p=0) ^∞ (((−1)^p )/(p!))∫_0 ^∞   (t^p /(t^2  +4π^2 (n+1)^2 ))dt....be continued...

lettakeatrywithseriesA=0arctanxe2πx1dxA=0e2πxarctanx1e2πxdx=0e2πxarctanxn=0e2nπxdx=n=00e2π(n+1)xarctanxdx=n=0AnAn=0e2π(n+1)xarctanxdx=byparts[e2π(n+1)x2π(n+1)arctanx]0+0e2π(n+1)x2π(n+1)×dx1+x2=12π(n+1)0e2π(n+1)x1+x2dx=2π(n+1)x=t12π(n+1)0et1+t24π2(n+1)2×dt2π(n+1)=14π2(n+1)20ett2+4π2(n+1)2×4π2(n+1)2dt=0ett2+4π2(n+1)2dt=01t2+4π2(n+1)2(p=0(t)pp!)dt=p=0(1)pp!0tpt2+4π2(n+1)2dt....becontinued...

Answered by mindispower last updated on 25/Oct/20

Abel plana formula  Σ_(m≥0) f(m)=∫_0 ^∞ f(x)dx+((f(0))/2)+i∫_0 ^∞ ((f(it)−f(−it))/(e^(2πt) −1))dt  f(x)=(1/((x+z)^2 ))⇒  Σ_(n≥0) (1/((n+z)^2 ))=∫^∞ _0 (1/((x+z)^2 ))dx+(1/(2z^2 ))+i∫_0 ^∞ (((1/((it+z)^2 ))−(1/((−it+z)^2 )))/(e^(2πt) −1))dt  =(1/z)+(1/(2z^2 ))+i∫_0 ^∞ ((−4itz)/((z^2 +t^2 )^2 (e^(2πt) −1)))dt  =(1/z)+(1/(2z^2 ))+2∫_0 ^∞ ((2tz)/((z^2 +t^2 )^2 (e^(2πt) −1)))dt  Σ_(n≥0) (1/((n+z)^2 ))=Ψ′(z)=(lnΓ(z))′′  we have  ln(Γ(z))′′=(1/z)+(1/(2z^2 ))+2∫_0 ^∞ ((2tz)/((z^2 +t^2 )^2 (e^(2πt) −1)))dt  by integrate  ⇒ln(Γ(z))′=ln(z)−(1/(2z))+2∫_0 ^∞ −(t/((z^2 +t^2 ))).(dt/((e^(2πt) −1)))+c  ln(Γ(z))=zln(z)−z−(1/2)ln(z)−2∫_0 ^∞ ∫(t/(z^2 +t^2 ))dz.(dt/(e^(2πt) −1))+cz+c′  =(z−(1/2))ln(z)+(c−1)z+2∫_0 ^∞ ((arctan((t/z)))/(e^(2πt) −1))dt+c′  ⇒[log(Γ(z))−(z−(1/2))ln(z)−(c−1)z−c′]=2∫((arctan((t/z)))/(e^(2πt) −1))  when z→∞?we muste have 0 bothe side  ⇒c=′((log(2π))/2),c=0“striling formula for Γ(z)”  ⇔  log(Γ(z))=(z−(1/2))ln(z)−z+((log(2π))/2)+2∫_0 ^∞ ((tan^(−1) ((t/z)))/(e^(2πt) −1))dt  for z=1  ⇒log(Γ(1))=−1+((log(2π))/2)+2∫_0 ^∞ ((tan^(−1) (t))/(e^(2πt) −1))dt  ⇒∫_0 ^∞ ((tan^(−1) (t))/(e^(2πt) −1))dt=((2−log(2π))/4)

Abelplanaformulam0f(m)=0f(x)dx+f(0)2+i0f(it)f(it)e2πt1dtf(x)=1(x+z)2n01(n+z)2=01(x+z)2dx+12z2+i01(it+z)21(it+z)2e2πt1dt=1z+12z2+i04itz(z2+t2)2(e2πt1)dt=1z+12z2+202tz(z2+t2)2(e2πt1)dtn01(n+z)2=Ψ(z)=(lnΓ(z))wehaveln(Γ(z))=1z+12z2+202tz(z2+t2)2(e2πt1)dtbyintegrateln(Γ(z))=ln(z)12z+20t(z2+t2).dt(e2πt1)+cln(Γ(z))=zln(z)z12ln(z)20tz2+t2dz.dte2πt1+cz+c=(z12)ln(z)+(c1)z+20arctan(tz)e2πt1dt+c[log(Γ(z))(z12)ln(z)(c1)zc]=2arctan(tz)e2πt1whenz?wemustehave0bothesidec=log(2π)2,c=0strilingformulaforΓ(z)log(Γ(z))=(z12)ln(z)z+log(2π)2+20tan1(tz)e2πt1dtforz=1log(Γ(1))=1+log(2π)2+20tan1(t)e2πt1dt0tan1(t)e2πt1dt=2log(2π)4

Commented by mnjuly1970 last updated on 25/Oct/20

peace be upon you mr power   .super nice    good for you...

peacebeuponyoumrpower.supernicegoodforyou...

Commented by mindispower last updated on 25/Oct/20

withe pleasur

withepleasur

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