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Question Number 33629 by naka3546 last updated on 20/Apr/18

Commented by math khazana by abdo last updated on 22/Apr/18

let put I = ∫_0 ^(π/2)      (dx/(1+a^2 tan^2 x))  .changement  tanx =t give I = ∫_0 ^∞       (1/(1+a^2 t^2 )) (dt/(1+t^2 )) ⇒  2I  =∫_(−∞) ^(+∞)     (dt/((1+t^2 )(1+a^2 t^2 ))) let introduce the  complex function ϕ(z) =  (1/((1+z^2 )(1+a^2 z^2 )))  let suppose a≠0 we have  ϕ(z) =  (1/((z−i)(z+i)( az−i)−az+i)))  =  (1/(a^2 (z−i)(z+i)(z−(i/a))(z +(i/a)))) so the poles of ϕ  are i,−i,(i/a),−(i/a)  case1  a>0  ∫_(−∞) ^(+∞)  ϕ(z)dz =2iπ( Res(ϕ,i) +Res(ϕ,(i/a)))  Res(ϕ,i) =   (1/(2i(1−a^2 )))  Res(ϕ, (i/a)) =   (1/(2a^2 (i/a)(1+((i/a))^2 ))) =  (1/(2ia(1−(1/a^2 )))) = (a^2 /(2ia(a^2 −1)))=(a/(2i(a^2 −1)))  ∫_(−∞) ^(+∞)   ϕ(z)dz = 2iπ(   (1/(2i(1−a^2 ))) −(a/(2i(1−a^2 ))))  = (π/(1−a^2 ))  −((2πa)/(1−a^2 )) = (π/(1−a^2 ))(1−a) = (π/(1+a))

letputI=0π2dx1+a2tan2x.changementtanx=tgiveI=011+a2t2dt1+t22I=+dt(1+t2)(1+a2t2)letintroducethecomplexfunctionφ(z)=1(1+z2)(1+a2z2)letsupposea0wehaveφ(z)=1(zi)(z+i)(azi)az+i)=1a2(zi)(z+i)(zia)(z+ia)sothepolesofφarei,i,ia,iacase1a>0+φ(z)dz=2iπ(Res(φ,i)+Res(φ,ia))Res(φ,i)=12i(1a2)Res(φ,ia)=12a2ia(1+(ia)2)=12ia(11a2)=a22ia(a21)=a2i(a21)+φ(z)dz=2iπ(12i(1a2)a2i(1a2))=π1a22πa1a2=π1a2(1a)=π1+a

Commented by math khazana by abdo last updated on 22/Apr/18

2I= (π/(1+a)) ⇒ I  =(π/(2(1+a)))  case2  a<0  ∫_(−∞) ^(+∞) ϕ(z)dz  =2iπ( Res(ϕ,i) +Res(ϕ,−(i/a)))  Res(ϕ,−(i/a)) =  (1/(a^2 (−2(i/a))(1−(1/a^2 ))))  =  ((a^2  )/(−2ia(a^2  −1))) =  (a^2 /(2ia(1−a^2 ))) = (a/(2i(1−a^2 )))  ∫_(−∞) ^(+∞)   ϕ(z)dz =2iπ(   (1/(2i(1−a^2 )))  +  (a/(2i(1−a^2 ))))  = (π/(1−a^2 ))  +((πa)/(1−a^2 )) = (π/(1−a^2 ))(1+a) = (π/(1−a)) ⇒  I = (π/(2(1−a)))  but we must study the specials?cases  a=+^− 1  and a=0 .

2I=π1+aI=π2(1+a)case2a<0+φ(z)dz=2iπ(Res(φ,i)+Res(φ,ia))Res(φ,ia)=1a2(2ia)(11a2)=a22ia(a21)=a22ia(1a2)=a2i(1a2)+φ(z)dz=2iπ(12i(1a2)+a2i(1a2))=π1a2+πa1a2=π1a2(1+a)=π1aI=π2(1a)butwemuststudythespecials?casesa=+1anda=0.

Answered by sma3l2996 last updated on 21/Apr/18

A=∫_0 ^(π/2) (dx/(1+a^2 tan^2 x))  let  t=atanx⇒dx=((adt)/(a^2 +t^2 ))  A=a∫_0 ^∞ (dt/((a^2 +t^2 )(1+t^2 )))  (1/((a^2 +t^2 )(1+t^2 )))=((kt+z)/(a^2 +t^2 ))+((rt+d)/(1+t^2 ))  with  k=r=0  and  d=−z=(1/(a^2 −1))  so  A=(a/(a^2 −1))∫_0 ^∞ ((1/(1+t^2 ))−(1/(a^2 +t^2 )))dt  =(a/(a^2 −1))(∫_0 ^∞ (dt/(1+t^2 ))−∫_0 ^∞ (dt/(a^2 (1+((t/a))^2 ))))  =(a/(a^2 −1))[tan^(−1) t]_0 ^∞ −(1/((a^2 −1)))∫_0 ^∞ (1/(1+((t/a))^2 ))d((t/a))  =((aπ)/(2(a^2 −1)))−(π/(2(a^2 −1)))=(π/(2(a^2 −1)))(a−1)  A=(π/(2(a+1)))

A=0π/2dx1+a2tan2xlett=atanxdx=adta2+t2A=a0dt(a2+t2)(1+t2)1(a2+t2)(1+t2)=kt+za2+t2+rt+d1+t2withk=r=0andd=z=1a21soA=aa210(11+t21a2+t2)dt=aa21(0dt1+t20dta2(1+(ta)2))=aa21[tan1t]01(a21)011+(ta)2d(ta)=aπ2(a21)π2(a21)=π2(a21)(a1)A=π2(a+1)

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