Grile de Integrale definite — Clasa a 12-a

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Teorie Integrale definite — Formule si exemple rezolvate

Probleme de Integrale definite

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Greu#1
Fie I=∫0πxsin⁡x1+cos⁡2x dxI = \int_{0}^{\pi} \frac{x \sin x}{1 + \cos^2 x} \, dx. Care este valoarea integralei II?
A) π24\frac{\pi^2}{4}
B) π22\frac{\pi^2}{2}
C) π2\pi^2
D) π28\frac{\pi^2}{8}

Explicație

Se utilizează proprietatea ∫0af(x) dx=∫0af(a−x) dx\int_{0}^{a} f(x) \, dx = \int_{0}^{a} f(a-x) \, dx. Aici a=πa = \pi. Atunci: I=∫0π(π−x)sin⁡(π−x)1+cos⁡2(π−x) dx=∫0π(π−x)sin⁡x1+cos⁡2x dx.I = \int_{0}^{\pi} \frac{(\pi - x) \sin(\pi - x)}{1 + \cos^2(\pi - x)} \, dx = \int_{0}^{\pi} \frac{(\pi - x) \sin x}{1 + \cos^2 x} \, dx. Adunând expresiile inițiale și cele transformate: I+I=∫0πxsin⁡x1+cos⁡2x dx+∫0π(π−x)sin⁡x1+cos⁡2x dx=∫0ππsin⁡x1+cos⁡2x dx.I + I = \int_{0}^{\pi} \frac{x \sin x}{1 + \cos^2 x} \, dx + \int_{0}^{\pi} \frac{(\pi - x) \sin x}{1 + \cos^2 x} \, dx = \int_{0}^{\pi} \frac{\pi \sin x}{1 + \cos^2 x} \, dx. Deci 2I=π∫0πsin⁡x1+cos⁡2x dx2I = \pi \int_{0}^{\pi} \frac{\sin x}{1 + \cos^2 x} \, dx. Se face substituția u=cos⁡xu = \cos x, du=−sin⁡x dxdu = -\sin x \, dx. Când x=0x=0, u=1u=1; când x=πx=\pi, u=−1u=-1. Atunci: ∫0πsin⁡x1+cos⁡2x dx=∫1−1−du1+u2=∫−11du1+u2=arctan⁡u∣−11=π4−(−π4)=π2.\int_{0}^{\pi} \frac{\sin x}{1 + \cos^2 x} \, dx = \int_{1}^{-1} \frac{-du}{1+u^2} = \int_{-1}^{1} \frac{du}{1+u^2} = \arctan u \Big|_{-1}^{1} = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}. Așadar, 2I=π⋅π2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, de unde rezultă I=π24I = \frac{\pi^2}{4}.
Greu#2
Să se calculeze integrala definită: I=∫0πxsin⁡x1+cos⁡2x dx\displaystyle I = \int_{0}^{\pi} \frac{x \sin x}{1 + \cos^2 x} \, dx.
A) π24\frac{\pi^2}{4}
B) π22\frac{\pi^2}{2}
C) π2\frac{\pi}{2}
D) π28\frac{\pi^2}{8}

Explicație

Fie I=∫0πxsin⁡x1+cos⁡2x dxI = \int_{0}^{\pi} \frac{x \sin x}{1 + \cos^2 x} \, dx. Se face schimbarea u=π−xu = \pi - x, deci du=−dxdu = -dx. Atunci: I=∫π0(π−u)sin⁡(π−u)1+cos⁡2(π−u)(−du)=∫0π(π−u)sin⁡u1+cos⁡2u du,I = \int_{\pi}^{0} \frac{(\pi - u) \sin(\pi - u)}{1 + \cos^2(\pi - u)} (-du) = \int_{0}^{\pi} \frac{(\pi - u) \sin u}{1 + \cos^2 u} \, du, deoarece sin⁡(π−u)=sin⁡u\sin(\pi - u) = \sin u și cos⁡(π−u)=−cos⁡u\cos(\pi - u) = -\cos u, deci cos⁡2(π−u)=cos⁡2u\cos^2(\pi - u) = \cos^2 u. Prin urmare: I=π∫0πsin⁡u1+cos⁡2u du−∫0πusin⁡u1+cos⁡2u du=πJ−I,I = \pi \int_{0}^{\pi} \frac{\sin u}{1 + \cos^2 u} \, du - \int_{0}^{\pi} \frac{u \sin u}{1 + \cos^2 u} \, du = \pi J - I, unde J=∫0πsin⁡u1+cos⁡2u duJ = \int_{0}^{\pi} \frac{\sin u}{1 + \cos^2 u} \, du. Rezultă că 2I=πJ2I = \pi J, deci I=π2JI = \frac{\pi}{2} J. Pentru calculul lui JJ, facem substituția t=cos⁡ut = \cos u, dt=−sin⁡u dudt = -\sin u \, du. Când u=0u=0, t=1t=1; când u=πu=\pi, t=−1t=-1. Atunci: J=∫1−1−dt1+t2=∫−11dt1+t2=arctan⁡t∣−11=arctan⁡(1)−arctan⁡(−1)=π4−(−π4)=π2.J = \int_{1}^{-1} \frac{-dt}{1+t^2} = \int_{-1}^{1} \frac{dt}{1+t^2} = \arctan t \Big|_{-1}^{1} = \arctan(1) - \arctan(-1) = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}. Înlocuind, obținem I=π2⋅π2=π24I = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.
Greu#3
Calculați ∫0πxsin⁡x1+cos⁡2x dx\displaystyle \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx.
A) π24\dfrac{\pi^2}{4}
B) π22\dfrac{\pi^2}{2}
C) π2\dfrac{\pi}{2}
D) π\pi

Explicație

Fie I=∫0πxsin⁡x1+cos⁡2x dxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. \ Aplicăm substituția x=π−tx = \pi - t: \ dx=−dtdx = -dt, iar când x=0x=0, t=πt=\pi; când x=πx=\pi, t=0t=0. Atunci: [ I = \int_{\pi}^{0} \frac{(\pi - t) \sin(\pi - t)}{1+\cos^2(\pi - t)} (-dt) = \int_{0}^{\pi} \frac{(\pi - t) \sin t}{1+\cos^2 t} , dt = \pi \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t} , dt - I. ] \ Deci 2I=π∫0πsin⁡x1+cos⁡2x dx2I = \pi \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Notăm J=∫0πsin⁡x1+cos⁡2x dxJ = \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Pentru a calcula JJ, facem substituția u=cos⁡xu = \cos x, du=−sin⁡x dxdu = -\sin x \, dx. \ Când x=0x=0, u=1u=1; când x=πx=\pi, u=−1u=-1. Atunci: [ J = \int_{1}^{-1} \frac{-du}{1+u^2} = \int_{-1}^{1} \frac{du}{1+u^2} = \arctan u \Big|_{-1}^{1} = \arctan(1) - \arctan(-1) = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}. ] \ Astfel, 2I=π⋅π2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, de unde I=π24I = \frac{\pi^2}{4}.
Greu#4
Calculați I=∫0π4ln⁡(1+tan⁡x) dxI = \int_0^{\frac{\pi}{4}} \ln(1+\tan x) \, dx.
A) π8ln⁡2\frac{\pi}{8} \ln 2
B) π4ln⁡2\frac{\pi}{4} \ln 2
C) π2ln⁡2\frac{\pi}{2} \ln 2
D) ln⁡2\ln 2

Explicație

Fie I=∫0π4ln⁡(1+tan⁡x) dxI = \int_0^{\frac{\pi}{4}} \ln(1+\tan x) \, dx. Se aplică substituția u=π4−xu = \frac{\pi}{4} - x, deci du=−dxdu = -dx. Limitele devin: când x=0x=0, u=π4u=\frac{\pi}{4}; când x=π4x=\frac{\pi}{4}, u=0u=0. Atunci: I=∫π40ln⁡(1+tan⁡(π4−u))(−du)=∫0π4ln⁡(1+tan⁡(π4−u))du.I = \int_{\frac{\pi}{4}}^0 \ln\left(1+\tan\left(\frac{\pi}{4}-u\right)\right) (-du) = \int_0^{\frac{\pi}{4}} \ln\left(1+\tan\left(\frac{\pi}{4}-u\right)\right) du. Se știe că tan⁡(π4−u)=1−tan⁡u1+tan⁡u\tan\left(\frac{\pi}{4}-u\right) = \frac{1-\tan u}{1+\tan u}. Înlocuind: I=∫0π4ln⁡(1+1−tan⁡u1+tan⁡u)du=∫0π4ln⁡(1+tan⁡u+1−tan⁡u1+tan⁡u)du=∫0π4ln⁡(21+tan⁡u)du.I = \int_0^{\frac{\pi}{4}} \ln\left(1+\frac{1-\tan u}{1+\tan u}\right) du = \int_0^{\frac{\pi}{4}} \ln\left(\frac{1+\tan u + 1 - \tan u}{1+\tan u}\right) du = \int_0^{\frac{\pi}{4}} \ln\left(\frac{2}{1+\tan u}\right) du. Folosind proprietățile logaritmului: ln⁡(21+tan⁡u)=ln⁡2−ln⁡(1+tan⁡u)\ln\left(\frac{2}{1+\tan u}\right) = \ln 2 - \ln(1+\tan u). Astfel: I=∫0π4(ln⁡2−ln⁡(1+tan⁡u))du=ln⁡2⋅π4−∫0π4ln⁡(1+tan⁡u) du.I = \int_0^{\frac{\pi}{4}} \left(\ln 2 - \ln(1+\tan u)\right) du = \ln 2 \cdot \frac{\pi}{4} - \int_0^{\frac{\pi}{4}} \ln(1+\tan u) \, du. Dar ultima integrală este exact II, deci: I=π4ln⁡2−I  ⟹  2I=π4ln⁡2  ⟹  I=π8ln⁡2.I = \frac{\pi}{4} \ln 2 - I \implies 2I = \frac{\pi}{4} \ln 2 \implies I = \frac{\pi}{8} \ln 2.
Greu#5
Calculați integrala definită ∫0πxsin⁡x1+cos⁡2x dx\displaystyle \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx.
A) π24\frac{\pi^2}{4}
B) π22\frac{\pi^2}{2}
C) π28\frac{\pi^2}{8}
D) π22\frac{\pi^2}{\sqrt{2}}

Explicație

Notăm I=∫0πxsin⁡x1+cos⁡2x dxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. Efectuăm substituția x=π−tx = \pi - t, deci dx=−dtdx = -dt. Limitele devin: când x=0x=0, t=πt=\pi; când x=πx=\pi, t=0t=0. Atunci: I=∫π0(π−t)sin⁡(π−t)1+cos⁡2(π−t)(−dt)=∫0π(π−t)sin⁡t1+cos⁡2t dt=π∫0πsin⁡t1+cos⁡2t dt−I.I = \int_{\pi}^{0} \frac{(\pi - t) \sin(\pi - t)}{1+\cos^2(\pi - t)} (-dt) = \int_{0}^{\pi} \frac{(\pi - t) \sin t}{1+\cos^2 t} \, dt = \pi \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t} \, dt - I. Obținem 2I=π∫0πsin⁡t1+cos⁡2t dt2I = \pi \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t} \, dt. Calculăm integrala J=∫0πsin⁡t1+cos⁡2t dtJ = \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t} \, dt prin substituția u=cos⁡tu = \cos t, du=−sin⁡t dtdu = -\sin t \, dt: J=∫1−1−du1+u2=∫−11du1+u2=arctan⁡u∣−11=arctan⁡(1)−arctan⁡(−1)=π4−(−π4)=π2.J = \int_{1}^{-1} \frac{-du}{1+u^2} = \int_{-1}^{1} \frac{du}{1+u^2} = \arctan u \Big|_{-1}^{1} = \arctan(1) - \arctan(-1) = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}. Așadar, 2I=π⋅π2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, deci I=π24I = \frac{\pi^2}{4}.
Greu#6
Calculați ∫0πxsin⁡x1+cos⁡2x dx\displaystyle \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx.
A) π24\dfrac{\pi^2}{4}
B) π22\dfrac{\pi^2}{2}
C) π2\pi^2
D) π28\dfrac{\pi^2}{8}

Explicație

Fie I=∫0πxsin⁡x1+cos⁡2x dxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. Aplicăm substituția u=π−xu = \pi - x; atunci du=−dxdu = -dx, iar limitele devin de la π\pi la 00. Avem: I=∫π0(π−u)sin⁡(π−u)1+cos⁡2(π−u)(−du)=∫0π(π−u)sin⁡u1+cos⁡2u du=π∫0πsin⁡u1+cos⁡2u du−I.I = \int_{\pi}^{0} \frac{(\pi - u) \sin(\pi - u)}{1+\cos^2(\pi - u)} (-du) = \int_{0}^{\pi} \frac{(\pi - u) \sin u}{1+\cos^2 u} \, du = \pi \int_{0}^{\pi} \frac{\sin u}{1+\cos^2 u} \, du - I. Deci 2I=π∫0πsin⁡x1+cos⁡2x dx2I = \pi \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Pentru a calcula această integrală, notăm t=cos⁡xt = \cos x, dt=−sin⁡x dxdt = -\sin x \, dx. Când x=0x = 0, t=1t = 1; când x=πx = \pi, t=−1t = -1. Atunci: ∫0πsin⁡x1+cos⁡2x dx=∫1−1−dt1+t2=∫−11dt1+t2=arctan⁡t∣−11=π4−(−π4)=π2.\int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx = \int_{1}^{-1} \frac{-dt}{1+t^2} = \int_{-1}^{1} \frac{dt}{1+t^2} = \arctan t \Big|_{-1}^{1} = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}. Prin urmare, 2I=π⋅π2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, de unde I=π24I = \frac{\pi^2}{4}.
Greu#7
Calculați ∫01ln⁡(1+x)1+x2 dx\displaystyle \int_0^1 \frac{\ln(1+x)}{1+x^2} \, dx.
A) π8ln⁡2\dfrac{\pi}{8}\ln 2
B) π4ln⁡2\dfrac{\pi}{4}\ln 2
C) π2ln⁡2\dfrac{\pi}{2}\ln 2
D) π6ln⁡2\dfrac{\pi}{6}\ln 2

Explicație

Considerăm I=∫01ln⁡(1+x)1+x2dxI = \int_0^1 \frac{\ln(1+x)}{1+x^2} dx. Efectuăm substituția x=tan⁡tx = \tan t, cu dx=sec⁡2t dtdx = \sec^2 t\, dt. Limitele devin: x=0⇒t=0x=0 \Rightarrow t=0, x=1⇒t=π4x=1 \Rightarrow t=\frac{\pi}{4}. Atunci: [ I = \int_0^{\pi/4} \frac{\ln(1+\tan t)}{1+\tan^2 t} \sec^2 t, dt = \int_0^{\pi/4} \ln(1+\tan t), dt. ] Folosim schimbarea t=π4−ut = \frac{\pi}{4} - u, deci dt=−dudt = -du, iar limitele devin: t=0⇒u=π4t=0 \Rightarrow u=\frac{\pi}{4}, t=π4⇒u=0t=\frac{\pi}{4} \Rightarrow u=0. Atunci: [ I = \int_{\pi/4}^{0} \ln\left(1+\tan\left(\frac{\pi}{4}-u\right)\right)(-du) = \int_0^{\pi/4} \ln\left(1+\tan\left(\frac{\pi}{4}-u\right)\right) du. ] Calculăm: tan⁡(π4−u)=1−tan⁡u1+tan⁡u\tan\left(\frac{\pi}{4}-u\right) = \frac{1-\tan u}{1+\tan u}, deci [ 1+\tan\left(\frac{\pi}{4}-u\right) = 1+\frac{1-\tan u}{1+\tan u} = \frac{2}{1+\tan u}. ] Înlocuind: [ I = \int_0^{\pi/4} \ln\left(\frac{2}{1+\tan u}\right) du = \int_0^{\pi/4} \left(\ln 2 - \ln(1+\tan u)\right) du = \frac{\pi}{4}\ln 2 - \int_0^{\pi/4} \ln(1+\tan u), du. ] Dar ultima integrală este tocmai II (cu variabila mută uu). Deci: [ I = \frac{\pi}{4}\ln 2 - I \Rightarrow 2I = \frac{\pi}{4}\ln 2 \Rightarrow I = \frac{\pi}{8}\ln 2. ]
Greu#8
Calculați I=∫0πxsin⁡x1+cos⁡2x dxI = \int_0^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx.
A) π28\frac{\pi^2}{8}
B) π24\frac{\pi^2}{4}
C) π22\frac{\pi^2}{2}
D) π2\frac{\pi}{2}

Explicație

  1. Se notează I=∫0πxsin⁡x1+cos⁡2x dxI = \int_0^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx.\n2. Se aplică substituția u=π−xu = \pi - x. Atunci du=−dxdu = -dx, sin⁡(π−u)=sin⁡u\sin(\pi-u)=\sin u, cos⁡(π−u)=−cos⁡u\cos(\pi-u) = -\cos u, deci 1+cos⁡2(π−u)=1+cos⁡2u1+\cos^2(\pi-u)=1+\cos^2 u. Limitele se schimbă: x=0⇒u=πx=0 \Rightarrow u=\pi, x=π⇒u=0x=\pi \Rightarrow u=0.\nI=∫π0(π−u)sin⁡u1+cos⁡2u(−du)=∫0π(π−u)sin⁡u1+cos⁡2u du=π∫0πsin⁡u1+cos⁡2u du−I.I = \int_{\pi}^0 \frac{(\pi-u) \sin u}{1+\cos^2 u} (-du) = \int_0^{\pi} \frac{(\pi-u) \sin u}{1+\cos^2 u} \, du = \pi \int_0^{\pi} \frac{\sin u}{1+\cos^2 u} \, du - I.\n3. Din egalitatea I=π∫0πsin⁡x1+cos⁡2x dx−II = \pi \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx - I, rezultă 2I=π∫0πsin⁡x1+cos⁡2x dx2I = \pi \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx, deci I=π2∫0πsin⁡x1+cos⁡2x dxI = \frac{\pi}{2} \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx.\n4. Se calculează J=∫0πsin⁡x1+cos⁡2x dxJ = \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Cu substituția t=cos⁡xt = \cos x, dt=−sin⁡x dxdt = -\sin x \, dx: J=∫x=0πsin⁡x1+cos⁡2x dx=∫t=1−1−dt1+t2=∫−11dt1+t2=arctan⁡t∣−11=π4−(−π4)=π2.J = \int_{x=0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx = \int_{t=1}^{-1} \frac{-dt}{1+t^2} = \int_{-1}^{1} \frac{dt}{1+t^2} = \arctan t \Big|_{-1}^{1} = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}.\n5. Înlocuind: I=π2⋅π2=π24I = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.
Greu#9
Calculați ∫0π4ln⁡(1+tan⁡x) dx\int_{0}^{\frac{\pi}{4}} \ln(1+\tan x) \, dx.
A) π8ln⁡2\frac{\pi}{8} \ln 2
B) π4ln⁡2\frac{\pi}{4} \ln 2
C) 12ln⁡2\frac{1}{2} \ln 2
D) π2ln⁡2\frac{\pi}{2} \ln 2

Explicație

Fie I=∫0π4ln⁡(1+tan⁡x) dxI = \int_{0}^{\frac{\pi}{4}} \ln(1+\tan x) \, dx. Efectuăm schimbarea de variabilă y=π4−xy = \frac{\pi}{4} - x, deci dx=−dydx = -dy. Limitele devin: când x=0x=0, y=π4y=\frac{\pi}{4}; când x=π4x=\frac{\pi}{4}, y=0y=0. Atunci: I=∫π40ln⁡(1+tan⁡(π4−y))(−dy)=∫0π4ln⁡(1+tan⁡(π4−y)) dy.I = \int_{\frac{\pi}{4}}^{0} \ln(1+\tan(\frac{\pi}{4} - y)) (-dy) = \int_{0}^{\frac{\pi}{4}} \ln(1+\tan(\frac{\pi}{4} - y)) \, dy. Folosim identitatea trigonometrică: tan⁡(π4−y)=1−tan⁡y1+tan⁡y.\tan(\frac{\pi}{4} - y) = \frac{1 - \tan y}{1 + \tan y}. Atunci: 1+tan⁡(π4−y)=1+1−tan⁡y1+tan⁡y=1+tan⁡y+1−tan⁡y1+tan⁡y=21+tan⁡y.1+\tan(\frac{\pi}{4} - y) = 1 + \frac{1 - \tan y}{1 + \tan y} = \frac{1+\tan y + 1 - \tan y}{1+\tan y} = \frac{2}{1+\tan y}. Înlocuim: I=∫0π4ln⁡(21+tan⁡y)dy=∫0π4[ln⁡2−ln⁡(1+tan⁡y)] dy=∫0π4ln⁡2 dy−∫0π4ln⁡(1+tan⁡y) dy=π4ln⁡2−I.I = \int_{0}^{\frac{\pi}{4}} \ln\left(\frac{2}{1+\tan y}\right) dy = \int_{0}^{\frac{\pi}{4}} [\ln 2 - \ln(1+\tan y)] \, dy = \int_{0}^{\frac{\pi}{4}} \ln 2 \, dy - \int_{0}^{\frac{\pi}{4}} \ln(1+\tan y) \, dy = \frac{\pi}{4}\ln 2 - I. Obținem ecuația: I=π4ln⁡2−I⇒2I=π4ln⁡2⇒I=π8ln⁡2I = \frac{\pi}{4}\ln 2 - I \Rightarrow 2I = \frac{\pi}{4}\ln 2 \Rightarrow I = \frac{\pi}{8}\ln 2.
Greu#10
Calculați integrala definită ∫0πxsin⁡x1+cos⁡2x dx\displaystyle \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x}\,dx.
A) π24\frac{\pi^2}{4}
B) π22\frac{\pi^2}{2}
C) π28\frac{\pi^2}{8}
D) πln⁡2\pi \ln 2

Explicație

Fie I=∫0πxsin⁡x1+cos⁡2x dxI=\int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x}\,dx. Aplicăm substituția x=π−tx = \pi - t; atunci dx=−dtdx = -dt, iar limitele devin: pentru x=0x=0, t=πt=\pi; pentru x=πx=\pi, t=0t=0. Obținem: I=∫π0(π−t)sin⁡(π−t)1+cos⁡2(π−t)(−dt)=∫0π(π−t)sin⁡t1+cos⁡2t dt=π∫0πsin⁡t1+cos⁡2t dt−I.I = \int_{\pi}^{0} \frac{(\pi - t) \sin(\pi - t)}{1+\cos^2(\pi - t)} (-dt) = \int_{0}^{\pi} \frac{(\pi - t) \sin t}{1+\cos^2 t}\,dt = \pi \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t}\,dt - I. Deci 2I=π∫0πsin⁡t1+cos⁡2t dt2I = \pi \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t}\,dt, adică I=π2∫0πsin⁡t1+cos⁡2t dtI = \frac{\pi}{2} \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t}\,dt. Calculăm J=∫0πsin⁡t1+cos⁡2t dtJ = \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t}\,dt cu substituția u=cos⁡tu = \cos t, du=−sin⁡t dtdu = -\sin t\,dt. Pentru t=0t=0, u=1u=1; pentru t=πt=\pi, u=−1u=-1. Atunci: J=∫1−1−du1+u2=∫−11du1+u2=arctan⁡u∣−11=arctan⁡(1)−arctan⁡(−1)=π4−(−π4)=π2.J = \int_{1}^{-1} \frac{-du}{1+u^2} = \int_{-1}^{1} \frac{du}{1+u^2} = \arctan u \Big|_{-1}^{1} = \arctan(1) - \arctan(-1) = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}. Prin urmare, I=π2⋅π2=π24I = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.
Greu#11
Calculați integrala definită: ∫01ln⁡(1+x)1+x2 dx\displaystyle \int_0^1 \frac{\ln(1+x)}{1+x^2} \, dx.
A) πln⁡24\dfrac{\pi \ln 2}{4}
B) πln⁡28\dfrac{\pi \ln 2}{8}
C) πln⁡22\dfrac{\pi \ln 2}{2}
D) ln⁡24\dfrac{\ln 2}{4}

Explicație

Fie I=∫01ln⁡(1+x)1+x2 dxI = \int_0^1 \frac{\ln(1+x)}{1+x^2} \, dx.\nSe aplică substituția x=1−t1+tx = \frac{1-t}{1+t}; atunci dx=−2(1+t)2 dtdx = -\frac{2}{(1+t)^2}\, dt, iar limitele devin: x=0⇒t=1x=0 \Rightarrow t=1, x=1⇒t=0x=1 \Rightarrow t=0.\nSe obține: 1+x2=2(1+t2)(1+t)21+x^2 = \frac{2(1+t^2)}{(1+t)^2} și ln⁡(1+x)=ln⁡2−ln⁡(1+t)\ln(1+x) = \ln 2 - \ln(1+t).\nÎnlocuind:\nI=∫10ln⁡2−ln⁡(1+t)2(1+t2)(1+t)2⋅(−2(1+t)2)dt=∫10ln⁡2−ln⁡(1+t)1+t2(−1)dt=∫01ln⁡2−ln⁡(1+t)1+t2dtI = \int_1^0 \frac{\ln 2 - \ln(1+t)}{\frac{2(1+t^2)}{(1+t)^2}} \cdot \left(-\frac{2}{(1+t)^2}\right) dt = \int_1^0 \frac{\ln 2 - \ln(1+t)}{1+t^2} (-1) dt = \int_0^1 \frac{\ln 2 - \ln(1+t)}{1+t^2} dt.\nAstfel, I=ln⁡2∫01dt1+t2−∫01ln⁡(1+t)1+t2dt=ln⁡2⋅π4−II = \ln 2 \int_0^1 \frac{dt}{1+t^2} - \int_0^1 \frac{\ln(1+t)}{1+t^2} dt = \ln 2 \cdot \frac{\pi}{4} - I.\nRezultă 2I=πln⁡242I = \frac{\pi \ln 2}{4}, deci I=πln⁡28I = \frac{\pi \ln 2}{8}.
Greu#12
Calculați ∫0πxsin⁡x1+cos⁡2x dx\int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx.
A) π28\frac{\pi^2}{8}
B) π24\frac{\pi^2}{4}
C) π22\frac{\pi^2}{2}
D) π2\pi^2

Explicație

Notăm I=∫0πxsin⁡x1+cos⁡2x dxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. Aplicăm substituția u=π−xu = \pi - x: I=∫π0(π−u)sin⁡(π−u)1+cos⁡2(π−u)(−du)=∫0π(π−u)sin⁡u1+cos⁡2u du=∫0π(π−x)sin⁡x1+cos⁡2x dx.I = \int_{\pi}^{0} \frac{(\pi - u) \sin(\pi - u)}{1+\cos^2(\pi - u)} (-du) = \int_{0}^{\pi} \frac{(\pi - u) \sin u}{1+\cos^2 u} \, du = \int_{0}^{\pi} \frac{(\pi - x) \sin x}{1+\cos^2 x} \, dx. Adunăm cele două expresii pentru II: 2I=∫0πxsin⁡x1+cos⁡2x dx+∫0π(π−x)sin⁡x1+cos⁡2x dx=∫0ππsin⁡x1+cos⁡2x dx=π∫0πsin⁡x1+cos⁡2x dx.2I = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx + \int_{0}^{\pi} \frac{(\pi - x) \sin x}{1+\cos^2 x} \, dx = \int_{0}^{\pi} \frac{\pi \sin x}{1+\cos^2 x} \, dx = \pi \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Calculăm J=∫0πsin⁡x1+cos⁡2x dxJ = \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx cu substituția t=cos⁡xt = \cos x, dt=−sin⁡x dxdt = -\sin x \, dx: J=∫1−1−dt1+t2=∫−11dt1+t2=arctan⁡t∣−11=arctan⁡(1)−arctan⁡(−1)=π4−(−π4)=π2.J = \int_{1}^{-1} \frac{-dt}{1+t^2} = \int_{-1}^{1} \frac{dt}{1+t^2} = \arctan t \Big|_{-1}^{1} = \arctan(1) - \arctan(-1) = \frac{\pi}{4} - \left(-\frac{\pi}{4}\right) = \frac{\pi}{2}. Obținem 2I=π⋅π2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, deci I=π24I = \frac{\pi^2}{4}.

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