Grile de Integrale definite — Clasa a 12-a

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Teorie Integrale definite — Formule si exemple rezolvate

Probleme de Integrale definite

286 exerciții cu rezolvare pas cu pas

Greu#1
Fie I=0πxsinx1+cos2xdxI = \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(ax)dx\int_{0}^{a} f(x) \, dx = \int_{0}^{a} f(a-x) \, dx. Aici a=πa = \pi. Atunci: I=0π(πx)sin(πx)1+cos2(πx)dx=0π(πx)sinx1+cos2xdx.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=0πxsinx1+cos2xdx+0π(πx)sinx1+cos2xdx=0ππsinx1+cos2xdx.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=π0πsinx1+cos2xdx2I = \pi \int_{0}^{\pi} \frac{\sin x}{1 + \cos^2 x} \, dx. Se face substituția u=cosxu = \cos x, du=sinxdxdu = -\sin x \, dx. Când x=0x=0, u=1u=1; când x=πx=\pi, u=1u=-1. Atunci: 0πsinx1+cos2xdx=11du1+u2=11du1+u2=arctanu11=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=ππ2=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=0πxsinx1+cos2xdx\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=0πxsinx1+cos2xdxI = \int_{0}^{\pi} \frac{x \sin x}{1 + \cos^2 x} \, dx. Se face schimbarea u=πxu = \pi - x, deci du=dxdu = -dx. Atunci: I=π0(πu)sin(πu)1+cos2(πu)(du)=0π(πu)sinu1+cos2udu,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(πu)=sinu\sin(\pi - u) = \sin u și cos(πu)=cosu\cos(\pi - u) = -\cos u, deci cos2(πu)=cos2u\cos^2(\pi - u) = \cos^2 u. Prin urmare: I=π0πsinu1+cos2udu0πusinu1+cos2udu=πJI,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=0πsinu1+cos2uduJ = \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=cosut = \cos u, dt=sinududt = -\sin u \, du. Când u=0u=0, t=1t=1; când u=πu=\pi, t=1t=-1. Atunci: J=11dt1+t2=11dt1+t2=arctant11=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=π2π2=π24I = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.
Greu#3
Calculați 0πxsinx1+cos2xdx\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=0πxsinx1+cos2xdxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. \ Aplicăm substituția x=πtx = \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=π0πsinx1+cos2xdx2I = \pi \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Notăm J=0πsinx1+cos2xdxJ = \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Pentru a calcula JJ, facem substituția u=cosxu = \cos x, du=sinxdxdu = -\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=ππ2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, de unde I=π24I = \frac{\pi^2}{4}.
Greu#4
Calculați I=0π4ln(1+tanx)dxI = \int_0^{\frac{\pi}{4}} \ln(1+\tan x) \, dx.
A) π8ln2\frac{\pi}{8} \ln 2
B) π4ln2\frac{\pi}{4} \ln 2
C) π2ln2\frac{\pi}{2} \ln 2
D) ln2\ln 2

Explicație

Fie I=0π4ln(1+tanx)dxI = \int_0^{\frac{\pi}{4}} \ln(1+\tan x) \, dx. Se aplică substituția u=π4xu = \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(π4u))(du)=0π4ln(1+tan(π4u))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(π4u)=1tanu1+tanu\tan\left(\frac{\pi}{4}-u\right) = \frac{1-\tan u}{1+\tan u}. Înlocuind: I=0π4ln(1+1tanu1+tanu)du=0π4ln(1+tanu+1tanu1+tanu)du=0π4ln(21+tanu)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+tanu)=ln2ln(1+tanu)\ln\left(\frac{2}{1+\tan u}\right) = \ln 2 - \ln(1+\tan u). Astfel: I=0π4(ln2ln(1+tanu))du=ln2π40π4ln(1+tanu)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=π4ln2I    2I=π4ln2    I=π8ln2.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 0πxsinx1+cos2xdx\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=0πxsinx1+cos2xdxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. Efectuăm substituția x=πtx = \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(πt)sin(πt)1+cos2(πt)(dt)=0π(πt)sint1+cos2tdt=π0πsint1+cos2tdtI.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=π0πsint1+cos2tdt2I = \pi \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t} \, dt. Calculăm integrala J=0πsint1+cos2tdtJ = \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t} \, dt prin substituția u=costu = \cos t, du=sintdtdu = -\sin t \, dt: J=11du1+u2=11du1+u2=arctanu11=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=ππ2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, deci I=π24I = \frac{\pi^2}{4}.
Greu#6
Calculați 0πxsinx1+cos2xdx\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=0πxsinx1+cos2xdxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. Aplicăm substituția u=πxu = \pi - x; atunci du=dxdu = -dx, iar limitele devin de la π\pi la 00. Avem: I=π0(πu)sin(πu)1+cos2(πu)(du)=0π(πu)sinu1+cos2udu=π0πsinu1+cos2uduI.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=π0πsinx1+cos2xdx2I = \pi \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Pentru a calcula această integrală, notăm t=cosxt = \cos x, dt=sinxdxdt = -\sin x \, dx. Când x=0x = 0, t=1t = 1; când x=πx = \pi, t=1t = -1. Atunci: 0πsinx1+cos2xdx=11dt1+t2=11dt1+t2=arctant11=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=ππ2=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+x2dx\displaystyle \int_0^1 \frac{\ln(1+x)}{1+x^2} \, dx.
A) π8ln2\dfrac{\pi}{8}\ln 2
B) π4ln2\dfrac{\pi}{4}\ln 2
C) π2ln2\dfrac{\pi}{2}\ln 2
D) π6ln2\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=tantx = \tan t, cu dx=sec2tdtdx = \sec^2 t\, dt. Limitele devin: x=0t=0x=0 \Rightarrow t=0, x=1t=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=π4ut = \frac{\pi}{4} - u, deci dt=dudt = -du, iar limitele devin: t=0u=π4t=0 \Rightarrow u=\frac{\pi}{4}, t=π4u=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(π4u)=1tanu1+tanu\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=0πxsinx1+cos2xdxI = \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=0πxsinx1+cos2xdxI = \int_0^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx.\n2. Se aplică substituția u=πxu = \pi - x. Atunci du=dxdu = -dx, sin(πu)=sinu\sin(\pi-u)=\sin u, cos(πu)=cosu\cos(\pi-u) = -\cos u, deci 1+cos2(πu)=1+cos2u1+\cos^2(\pi-u)=1+\cos^2 u. Limitele se schimbă: x=0u=πx=0 \Rightarrow u=\pi, x=πu=0x=\pi \Rightarrow u=0.\nI=π0(πu)sinu1+cos2u(du)=0π(πu)sinu1+cos2udu=π0πsinu1+cos2uduI.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=π0πsinx1+cos2xdxII = \pi \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx - I, rezultă 2I=π0πsinx1+cos2xdx2I = \pi \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx, deci I=π20πsinx1+cos2xdxI = \frac{\pi}{2} \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx.\n4. Se calculează J=0πsinx1+cos2xdxJ = \int_0^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx. Cu substituția t=cosxt = \cos x, dt=sinxdxdt = -\sin x \, dx: J=x=0πsinx1+cos2xdx=t=11dt1+t2=11dt1+t2=arctant11=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=π2π2=π24I = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.
Greu#9
Calculați 0π4ln(1+tanx)dx\int_{0}^{\frac{\pi}{4}} \ln(1+\tan x) \, dx.
A) π8ln2\frac{\pi}{8} \ln 2
B) π4ln2\frac{\pi}{4} \ln 2
C) 12ln2\frac{1}{2} \ln 2
D) π2ln2\frac{\pi}{2} \ln 2

Explicație

Fie I=0π4ln(1+tanx)dxI = \int_{0}^{\frac{\pi}{4}} \ln(1+\tan x) \, dx. Efectuăm schimbarea de variabilă y=π4xy = \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(π4y))(dy)=0π4ln(1+tan(π4y))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(π4y)=1tany1+tany.\tan(\frac{\pi}{4} - y) = \frac{1 - \tan y}{1 + \tan y}. Atunci: 1+tan(π4y)=1+1tany1+tany=1+tany+1tany1+tany=21+tany.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+tany)dy=0π4[ln2ln(1+tany)]dy=0π4ln2dy0π4ln(1+tany)dy=π4ln2I.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=π4ln2I2I=π4ln2I=π8ln2I = \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 0πxsinx1+cos2xdx\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) πln2\pi \ln 2

Explicație

Fie I=0πxsinx1+cos2xdxI=\int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x}\,dx. Aplicăm substituția x=πtx = \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(πt)sin(πt)1+cos2(πt)(dt)=0π(πt)sint1+cos2tdt=π0πsint1+cos2tdtI.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=π0πsint1+cos2tdt2I = \pi \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t}\,dt, adică I=π20πsint1+cos2tdtI = \frac{\pi}{2} \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t}\,dt. Calculăm J=0πsint1+cos2tdtJ = \int_{0}^{\pi} \frac{\sin t}{1+\cos^2 t}\,dt cu substituția u=costu = \cos t, du=sintdtdu = -\sin t\,dt. Pentru t=0t=0, u=1u=1; pentru t=πt=\pi, u=1u=-1. Atunci: J=11du1+u2=11du1+u2=arctanu11=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=π2π2=π24I = \frac{\pi}{2} \cdot \frac{\pi}{2} = \frac{\pi^2}{4}.
Greu#11
Calculați integrala definită: 01ln(1+x)1+x2dx\displaystyle \int_0^1 \frac{\ln(1+x)}{1+x^2} \, dx.
A) πln24\dfrac{\pi \ln 2}{4}
B) πln28\dfrac{\pi \ln 2}{8}
C) πln22\dfrac{\pi \ln 2}{2}
D) ln24\dfrac{\ln 2}{4}

Explicație

Fie I=01ln(1+x)1+x2dxI = \int_0^1 \frac{\ln(1+x)}{1+x^2} \, dx.\nSe aplică substituția x=1t1+tx = \frac{1-t}{1+t}; atunci dx=2(1+t)2dtdx = -\frac{2}{(1+t)^2}\, dt, iar limitele devin: x=0t=1x=0 \Rightarrow t=1, x=1t=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)=ln2ln(1+t)\ln(1+x) = \ln 2 - \ln(1+t).\nÎnlocuind:\nI=10ln2ln(1+t)2(1+t2)(1+t)2(2(1+t)2)dt=10ln2ln(1+t)1+t2(1)dt=01ln2ln(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=ln201dt1+t201ln(1+t)1+t2dt=ln2π4II = \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=πln242I = \frac{\pi \ln 2}{4}, deci I=πln28I = \frac{\pi \ln 2}{8}.
Greu#12
Calculați 0πxsinx1+cos2xdx\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=0πxsinx1+cos2xdxI = \int_{0}^{\pi} \frac{x \sin x}{1+\cos^2 x} \, dx. Aplicăm substituția u=πxu = \pi - x: I=π0(πu)sin(πu)1+cos2(πu)(du)=0π(πu)sinu1+cos2udu=0π(πx)sinx1+cos2xdx.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=0πxsinx1+cos2xdx+0π(πx)sinx1+cos2xdx=0ππsinx1+cos2xdx=π0πsinx1+cos2xdx.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=0πsinx1+cos2xdxJ = \int_{0}^{\pi} \frac{\sin x}{1+\cos^2 x} \, dx cu substituția t=cosxt = \cos x, dt=sinxdxdt = -\sin x \, dx: J=11dt1+t2=11dt1+t2=arctant11=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=ππ2=π222I = \pi \cdot \frac{\pi}{2} = \frac{\pi^2}{2}, deci I=π24I = \frac{\pi^2}{4}.

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