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Question Number 35832 by abdo mathsup 649 cc last updated on 24/May/18
find the value of  f(λ) = ∫_(−a) ^a    (dx/((λ +_ x^2 )^(3/2) ))  λ∈R .
$${find}\:{the}\:{value}\:{of}\:\:{f}\left(\lambda\right)\:=\:\int_{−{a}} ^{{a}} \:\:\:\frac{{dx}}{\left(\lambda\:+_{} {x}^{\mathrm{2}} \right)^{\frac{\mathrm{3}}{\mathrm{2}}} } \\ $$$$\lambda\in{R}\:. \\ $$
Commented by abdo.msup.com last updated on 25/May/18
case 1 ifλ>0 let use the changement  x=(√λ) tan(t)  f(λ) = ∫_(−arctan((a/λ))) ^(arctan((a/λ)))    ((√λ)/(λ^(3/2) (1+tan^2 (t))^(3/2) )) (1+tan^2 t)dt  =(1/λ)∫_(−arctan((a/( (√λ))))) ^(arctan( (a/( (√λ)))) )    (1/((1+tan^2 t)^(1/2) ))dt  = (2/λ) ∫_0 ^(arctan((a/( (√λ)))))   cos(t) dt  =(2/λ) [ sin(t)]_0 ^(arctan((a/( (√λ)))))   = (2/λ) sin(arctan((a/( (√λ)))))  but we have sin(arctanx) = (x/( (√(1+x^2 ))))  so sin(arctan((a/( (√λ))))) = (a/( (√λ) (√(1+(a^2 /λ)))))  = (a/( (√(λ +a^2 )))) ⇒f(λ) = ((2a)/(λ(√(λ+a^2 ))))
$${case}\:\mathrm{1}\:{if}\lambda>\mathrm{0}\:{let}\:{use}\:{the}\:{changement} \\ $$$${x}=\sqrt{\lambda}\:{tan}\left({t}\right) \\ $$$${f}\left(\lambda\right)\:=\:\int_{−{arctan}\left(\frac{{a}}{\lambda}\right)} ^{{arctan}\left(\frac{{a}}{\lambda}\right)} \:\:\:\frac{\sqrt{\lambda}}{\lambda^{\frac{\mathrm{3}}{\mathrm{2}}} \left(\mathrm{1}+{tan}^{\mathrm{2}} \left({t}\right)\right)^{\frac{\mathrm{3}}{\mathrm{2}}} }\:\left(\mathrm{1}+{tan}^{\mathrm{2}} {t}\right){dt} \\ $$$$=\frac{\mathrm{1}}{\lambda}\int_{−{arctan}\left(\frac{{a}}{\:\sqrt{\lambda}}\right)} ^{{arctan}\left(\:\frac{{a}}{\:\sqrt{\lambda}}\right)\:} \:\:\:\frac{\mathrm{1}}{\left(\mathrm{1}+{tan}^{\mathrm{2}} {t}\right)^{\frac{\mathrm{1}}{\mathrm{2}}} }{dt} \\ $$$$=\:\frac{\mathrm{2}}{\lambda}\:\int_{\mathrm{0}} ^{{arctan}\left(\frac{{a}}{\:\sqrt{\lambda}}\right)} \:\:{cos}\left({t}\right)\:{dt} \\ $$$$=\frac{\mathrm{2}}{\lambda}\:\left[\:{sin}\left({t}\right)\right]_{\mathrm{0}} ^{{arctan}\left(\frac{{a}}{\:\sqrt{\lambda}}\right)} \\ $$$$=\:\frac{\mathrm{2}}{\lambda}\:{sin}\left({arctan}\left(\frac{{a}}{\:\sqrt{\lambda}}\right)\right) \\ $$$${but}\:{we}\:{have}\:{sin}\left({arctanx}\right)\:=\:\frac{{x}}{\:\sqrt{\mathrm{1}+{x}^{\mathrm{2}} }} \\ $$$${so}\:{sin}\left({arctan}\left(\frac{{a}}{\:\sqrt{\lambda}}\right)\right)\:=\:\frac{{a}}{\:\sqrt{\lambda}\:\sqrt{\mathrm{1}+\frac{{a}^{\mathrm{2}} }{\lambda}}} \\ $$$$=\:\frac{{a}}{\:\sqrt{\lambda\:+{a}^{\mathrm{2}} }}\:\Rightarrow{f}\left(\lambda\right)\:=\:\frac{\mathrm{2}{a}}{\lambda\sqrt{\lambda+{a}^{\mathrm{2}} }} \\ $$
Commented by prof Abdo imad last updated on 25/May/18
case 2 if  λ<0 ⇒ −λ >0 let put α =−λ  f(λ) = ∫_(−a) ^a    (dx/((x^2  −α)^(3/2) ))  .changement x=(√α)ch(t)  give   f(λ) = ∫_(argch( ((−a)/( (√α))))) ^(argch( (a/( (√α)))))      (((√α)  sh(t))/(α^(3/2) ( ch^2 (t)−1)^(3/2) ))dt  = (1/α)∫_(argch(((−a)/( (√α))))) ^(argch( (a/( (√α)))))     ((sh(t))/(sh^3 (t)))dt   = (2/α) ∫_(argch( ((−a)/( (√α))))) ^(argch((a/( (√α)))))      (dt/(ch(2t)−1))  = (2/α) ∫_(ln( −(a/( (√κ)))  +(√( (a^2 /α) −1)))) ^(ln( (a/( (√α))) +(√( (a^2 /α)−1)))        (dt/(((e^(2t)  +e^(−2t) )/2) −1))  = (4/α) ∫_(ln(−(a/( (√α))) +(√( (a^2 /α)−1)))) ^(ln( (a/( (√α))) +(√((a^2 /α)−1))))      (dt/(e^(2t)  +e^(−2t)  −2)) ...  be continued...
$${case}\:\mathrm{2}\:{if}\:\:\lambda<\mathrm{0}\:\Rightarrow\:−\lambda\:>\mathrm{0}\:{let}\:{put}\:\alpha\:=−\lambda \\ $$$${f}\left(\lambda\right)\:=\:\int_{−{a}} ^{{a}} \:\:\:\frac{{dx}}{\left({x}^{\mathrm{2}} \:−\alpha\right)^{\frac{\mathrm{3}}{\mathrm{2}}} }\:\:.{changement}\:{x}=\sqrt{\alpha}{ch}\left({t}\right) \\ $$$${give}\: \\ $$$${f}\left(\lambda\right)\:=\:\int_{{argch}\left(\:\frac{−{a}}{\:\sqrt{\alpha}}\right)} ^{{argch}\left(\:\frac{{a}}{\:\sqrt{\alpha}}\right)} \:\:\:\:\:\frac{\sqrt{\alpha}\:\:{sh}\left({t}\right)}{\alpha^{\frac{\mathrm{3}}{\mathrm{2}}} \left(\:{ch}^{\mathrm{2}} \left({t}\right)−\mathrm{1}\right)^{\frac{\mathrm{3}}{\mathrm{2}}} }{dt} \\ $$$$=\:\frac{\mathrm{1}}{\alpha}\int_{{argch}\left(\frac{−{a}}{\:\sqrt{\alpha}}\right)} ^{{argch}\left(\:\frac{{a}}{\:\sqrt{\alpha}}\right)} \:\:\:\:\frac{{sh}\left({t}\right)}{{sh}^{\mathrm{3}} \left({t}\right)}{dt}\: \\ $$$$=\:\frac{\mathrm{2}}{\alpha}\:\int_{{argch}\left(\:\frac{−{a}}{\:\sqrt{\alpha}}\right)} ^{{argch}\left(\frac{{a}}{\:\sqrt{\alpha}}\right)} \:\:\:\:\:\frac{{dt}}{{ch}\left(\mathrm{2}{t}\right)−\mathrm{1}} \\ $$$$=\:\frac{\mathrm{2}}{\alpha}\:\int_{{ln}\left(\:−\frac{{a}}{\:\sqrt{\kappa}}\:\:+\sqrt{\:\frac{{a}^{\mathrm{2}} }{\alpha}\:−\mathrm{1}}\right)} ^{{ln}\left(\:\frac{{a}}{\:\sqrt{\alpha}}\:+\sqrt{\:\frac{{a}^{\mathrm{2}} }{\alpha}−\mathrm{1}}\right.} \:\:\:\:\:\:\:\frac{{dt}}{\frac{{e}^{\mathrm{2}{t}} \:+{e}^{−\mathrm{2}{t}} }{\mathrm{2}}\:−\mathrm{1}} \\ $$$$=\:\frac{\mathrm{4}}{\alpha}\:\int_{{ln}\left(−\frac{{a}}{\:\sqrt{\alpha}}\:+\sqrt{\:\frac{{a}^{\mathrm{2}} }{\alpha}−\mathrm{1}}\right)} ^{{ln}\left(\:\frac{{a}}{\:\sqrt{\alpha}}\:+\sqrt{\frac{{a}^{\mathrm{2}} }{\alpha}−\mathrm{1}}\right)} \:\:\:\:\:\frac{{dt}}{{e}^{\mathrm{2}{t}} \:+{e}^{−\mathrm{2}{t}} \:−\mathrm{2}}\:… \\ $$$${be}\:{continued}… \\ $$$$ \\ $$
Commented by prof Abdo imad last updated on 26/May/18
let find K=∫       (dt/(e^(2t)  +e^(−2t)  −2))  chamgement  e^(2t)  =u give  K = ∫  (1/(u +u^(−1)  −2)) (du/(2u))  =(1/2) ∫      (du/(u^2  +1 −2u)) =(1/2)∫   (du/((u−1)^2 ))  = −(1/(2(u−1)))  =((−1)/(2(e^(2t)  −1))) +c so  f(λ) = −(4/(2α)) [  (1/(e^(2t) −1))]_(ln(((−a)/( (√α))) +(√((a^2 /α)−1))) ^(ln( (a/( (√α))) +(√((a^2 /α) −1)))   = ((−2)/α){     (1/(((a/( (√α))) +(√((a^2 /α)−1))))) − (1/((−(a/( (√α)))+(√((a^2 /α) −1)))))  = (2/λ){     (1/(( (a/( (√(−λ)))) +(√(−(a^2 /λ)−1)))))−(1/((((−a)/( (√(−λ))))+(√(−(a^2 /λ)−1)))))  with λ<0 .
$${let}\:{find}\:{K}=\int\:\:\:\:\:\:\:\frac{{dt}}{{e}^{\mathrm{2}{t}} \:+{e}^{−\mathrm{2}{t}} \:−\mathrm{2}}\:\:{chamgement} \\ $$$${e}^{\mathrm{2}{t}} \:={u}\:{give}\:\:{K}\:=\:\int\:\:\frac{\mathrm{1}}{{u}\:+{u}^{−\mathrm{1}} \:−\mathrm{2}}\:\frac{{du}}{\mathrm{2}{u}} \\ $$$$=\frac{\mathrm{1}}{\mathrm{2}}\:\int\:\:\:\:\:\:\frac{{du}}{{u}^{\mathrm{2}} \:+\mathrm{1}\:−\mathrm{2}{u}}\:=\frac{\mathrm{1}}{\mathrm{2}}\int\:\:\:\frac{{du}}{\left({u}−\mathrm{1}\right)^{\mathrm{2}} } \\ $$$$=\:−\frac{\mathrm{1}}{\mathrm{2}\left({u}−\mathrm{1}\right)}\:\:=\frac{−\mathrm{1}}{\mathrm{2}\left({e}^{\mathrm{2}{t}} \:−\mathrm{1}\right)}\:+{c}\:{so} \\ $$$${f}\left(\lambda\right)\:=\:−\frac{\mathrm{4}}{\mathrm{2}\alpha}\:\left[\:\:\frac{\mathrm{1}}{{e}^{\mathrm{2}{t}} −\mathrm{1}}\right]_{{ln}\left(\frac{−{a}}{\:\sqrt{\alpha}}\:+\sqrt{\frac{{a}^{\mathrm{2}} }{\alpha}−\mathrm{1}}\right.} ^{{ln}\left(\:\frac{{a}}{\:\sqrt{\alpha}}\:+\sqrt{\frac{{a}^{\mathrm{2}} }{\alpha}\:−\mathrm{1}}\right.} \\ $$$$=\:\frac{−\mathrm{2}}{\alpha}\left\{\:\:\:\:\:\frac{\mathrm{1}}{\left(\frac{{a}}{\:\sqrt{\alpha}}\:+\sqrt{\frac{{a}^{\mathrm{2}} }{\alpha}−\mathrm{1}}\right)}\:−\:\frac{\mathrm{1}}{\left(−\frac{{a}}{\:\sqrt{\alpha}}+\sqrt{\frac{{a}^{\mathrm{2}} }{\alpha}\:−\mathrm{1}}\right)}\right. \\ $$$$=\:\frac{\mathrm{2}}{\lambda}\left\{\:\:\:\:\:\frac{\mathrm{1}}{\left(\:\frac{{a}}{\:\sqrt{−\lambda}}\:+\sqrt{−\frac{{a}^{\mathrm{2}} }{\lambda}−\mathrm{1}}\right)}−\frac{\mathrm{1}}{\left(\frac{−{a}}{\:\sqrt{−\lambda}}+\sqrt{−\frac{{a}^{\mathrm{2}} }{\lambda}−\mathrm{1}}\right)}\right. \\ $$$${with}\:\lambda<\mathrm{0}\:. \\ $$
Answered by tanmay.chaudhury50@gmail.com last updated on 24/May/18
x=(√λ) tanθ   dx=(√λ) sec^2 θ dθ  I=∫(((√λ) sec^2 θ dθ)/({λ(1+tan^2 θ)}^(3/2) ))  ∫(1/λ) ×((sec^2 θ)/(sec^3 θ))×(dθ/)  =(1/λ)∫cosθ dθ  =(1/λ)sinθ  now putting the limit  =(1/λ)×∣(x/((λ+x^2 )^(1/2)  ))∣_(−a) ^a   =(1/λ)×((2a)/((λ+a^2 )^(1/2) ))
$${x}=\sqrt{\lambda}\:{tan}\theta\:\:\:{dx}=\sqrt{\lambda}\:{sec}^{\mathrm{2}} \theta\:{d}\theta \\ $$$${I}=\int\frac{\sqrt{\lambda}\:{sec}^{\mathrm{2}} \theta\:{d}\theta}{\left\{\lambda\left(\mathrm{1}+{tan}^{\mathrm{2}} \theta\right)\right\}^{\frac{\mathrm{3}}{\mathrm{2}}} } \\ $$$$\int\frac{\mathrm{1}}{\lambda}\:×\frac{{sec}^{\mathrm{2}} \theta}{{sec}^{\mathrm{3}} \theta}×\frac{{d}\theta}{} \\ $$$$=\frac{\mathrm{1}}{\lambda}\int{cos}\theta\:{d}\theta \\ $$$$=\frac{\mathrm{1}}{\lambda}{sin}\theta\:\:{now}\:{putting}\:{the}\:{limit} \\ $$$$=\frac{\mathrm{1}}{\lambda}×\mid\frac{{x}}{\left(\lambda+{x}^{\mathrm{2}} \right)^{\frac{\mathrm{1}}{\mathrm{2}}} \:}\mid_{−{a}} ^{{a}} \\ $$$$=\frac{\mathrm{1}}{\lambda}×\frac{\mathrm{2}{a}}{\left(\lambda+{a}^{\mathrm{2}} \right)^{\frac{\mathrm{1}}{\mathrm{2}}} } \\ $$
Commented by abdo.msup.com last updated on 25/May/18
your answer is correct sir Tanmay  but you must study the case λ<0....
$${your}\:{answer}\:{is}\:{correct}\:{sir}\:{Tanmay} \\ $$$${but}\:{you}\:{must}\:{study}\:{the}\:{case}\:\lambda<\mathrm{0}…. \\ $$

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