Calculus 9e - Chapter 7.1 Integration by Parts Complete Exercises Study Guide

Core Principles of Integration by Parts

  • Fundamental Formula for Indefinite Integrals: Integration by parts is derived from the product rule for differentiation. For differentiable functions u(x)u(x) and v(x)v(x), the integration by parts formula is:   ∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du

  • Definite Integral Formula: When evaluating over a bounded interval [a,b][a, b], the formula incorporates evaluation limits:   ∫abu dv=[u(x)v(x)]ab−∫abv du=u(b)v(b)−u(a)v(a)−∫abv du\int_a^b u\,dv = [u(x)v(x)]_a^b - \int_a^b v\,du = u(b)v(b) - u(a)v(a) - \int_a^b v\,du

  • Strategy for Selecting uu and dvdv (LIATE Rule): A common heuristic for choosing uu prioritizes functions in the following order:

    1. Logarithmic functions (e.g., ln⁡(x)\ln(x))

    2. Inverse trigonometric functions (e.g., arcsin⁡(x)\arcsin(x), arctan⁡(x)\arctan(x))

    3. Algebraic functions (e.g., xnx^n, x\sqrt{x})

    4. Trigonometric functions (e.g., sin⁡(x)\sin(x), cos⁡(x)\cos(x))

    5. Exponential functions (e.g., exe^x, 3x3^x)

Guided Choice Exercises (Problems 1–4)

  • Exercise 1: Evaluate ∫xe2x dx\int x e^{2x}\,dx given u=xu = x and dv=e2x dxdv = e^{2x}\,dx.

    • Differentiating uu yields du=dxdu = dx.

    • Integrating dvdv yields v=12e2xv = \frac{1}{2} e^{2x}.

    • Applying the formula:     ∫xe2x dx=12xe2x−∫12e2x dx=12xe2x−14e2x+C=14e2x(2x−1)+C\int x e^{2x}\,dx = \frac{1}{2} x e^{2x} - \int \frac{1}{2} e^{2x}\,dx = \frac{1}{2} x e^{2x} - \frac{1}{4} e^{2x} + C = \frac{1}{4} e^{2x} (2x - 1) + C

  • Exercise 2: Evaluate ∫xln⁡(x) dx\int \sqrt{x} \ln(x)\,dx given u=ln⁡(x)u = \ln(x) and dv=x dxdv = \sqrt{x}\,dx.

    • Differentiating uu yields du = \frac{1}{x}\,dx$.\n - Integrating dv = x^{1/2}\,dxyieldsyieldsv = \frac{2}{3} x^{3/2}.\n - Applying the formula:\n    \int \sqrt{x} \ln(x)\,dx = \frac{2}{3} x^{3/2} \ln(x) - \int \frac{2}{3} x^{3/2} \cdot \frac{1}{x}\,dx = \frac{2}{3} x^{3/2} \ln(x) - \frac{2}{3} \int x^{1/2}\,dx = \frac{2}{3} x^{3/2} \ln(x) - \frac{4}{9} x^{3/2} + C\n\n- **Exercise 3:** Evaluate \int x \cos(4x)\,dxgivengivenu = xandanddv = \cos(4x)\,dx.\n - Differentiating uyieldsyieldsdu = dx$.

    • Integrating dvdv yields v=14sin⁡(4x)v = \frac{1}{4} \sin(4x).

    • Applying the formula:     ∫xcos⁡(4x) dx=14xsin⁡(4x)−∫14sin⁡(4x) dx=14xsin⁡(4x)+116cos⁡(4x)+C\int x \cos(4x)\,dx = \frac{1}{4} x \sin(4x) - \int \frac{1}{4} \sin(4x)\,dx = \frac{1}{4} x \sin(4x) + \frac{1}{16} \cos(4x) + C

  • Exercise 4: Evaluate ∫sin⁡−1(x) dx\int \sin^{-1}(x)\,dx given u=sin⁡−1(x)u = \sin^{-1}(x) and dv=dxdv = dx.

    • Differentiating uu yields du = \frac{1}{\sqrt{1 - x^2}}\,dx$.\n - Integrating dvyieldsyieldsv = x$.

    • Applying the formula:     ∫sin⁡−1(x) dx=xsin⁡−1(x)−∫x1−x2 dx=xsin⁡−1(x)+1−x2+C\int \sin^{-1}(x)\,dx = x \sin^{-1}(x) - \int \frac{x}{\sqrt{1 - x^2}}\,dx = x \sin^{-1}(x) + \sqrt{1 - x^2} + C

Standard Indefinite and Definite Integrals (Problems 5–42)

  • Exercise 5: ∫te2t dt\int t e^{2t}\,dt

    • Let u=t  ⟹  du=dtu = t \implies du = dt and dv=e2t dt  ⟹  v=12e2tdv = e^{2t}\,dt \implies v = \frac{1}{2} e^{2t}.

    • Result: 12te2t−14e2t+C\frac{1}{2} t e^{2t} - \frac{1}{4} e^{2t} + C

  • Exercise 6: ∫ye−y dy\int y e^{-y}\,dy

    • Let u=y  ⟹  du=dyu = y \implies du = dy and dv=e−y dy  ⟹  v=−e−ydv = e^{-y}\,dy \implies v = -e^{-y}.

    • Result: −ye−y−e−y+C=−e−y(y+1)+C-y e^{-y} - e^{-y} + C = -e^{-y} (y + 1) + C

  • Exercise 7: ∫xsin⁡(10x) dx\int x \sin(10x)\,dx

    • Let u=x  ⟹  du=dxu = x \implies du = dx and dv=sin⁡(10x) dx  ⟹  v=−110cos⁡(10x)dv = \sin(10x)\,dx \implies v = -\frac{1}{10} \cos(10x).

    • Result: −110xcos⁡(10x)+1100sin⁡(10x)+C- \frac{1}{10} x \cos(10x) + \frac{1}{100} \sin(10x) + C

  • Exercise 8: ∫(π−x)cos⁡(πx) dx\int (\pi - x) \cos(\pi x)\,dx

    • Let u=π−x  ⟹  du=−dxu = \pi - x \implies du = -dx and dv=cos⁡(πx) dx  ⟹  v=1πsin⁡(πx)dv = \cos(\pi x)\,dx \implies v = \frac{1}{\pi} \sin(\pi x).

    • Result: π−xπsin⁡(πx)−1π2cos⁡(πx)+C\frac{\pi - x}{\pi} \sin(\pi x) - \frac{1}{\pi^2} \cos(\pi x) + C

  • Exercise 9: ∫wln⁡(w) dw\int w \ln(w)\,dw

    • Let u=ln⁡(w)  ⟹  du=1w dwu = \ln(w) \implies du = \frac{1}{w}\,dw and dv=w dw  ⟹  v=12w2dv = w\,dw \implies v = \frac{1}{2} w^2.

    • Result: 12w2ln⁡(w)−14w2+C\frac{1}{2} w^2 \ln(w) - \frac{1}{4} w^2 + C

  • Exercise 10: ∫ln⁡(x)x2 dx\int \frac{\ln(x)}{x^2}\,dx

    • Let u=ln⁡(x)  ⟹  du=1x dxu = \ln(x) \implies du = \frac{1}{x}\,dx and dv=x−2 dx  ⟹  v=−x−1dv = x^{-2}\,dx \implies v = -x^{-1}.

    • Result: −ln⁡(x)x−1x+C- \frac{\ln(x)}{x} - \frac{1}{x} + C

  • Exercise 11: ∫(x2+2x)cos⁡(x) dx\int (x^2 + 2x) \cos(x)\,dx

    • Requires integration by parts twice:

    1. First pass: u=x2+2x  ⟹  du=(2x+2) dxu = x^2 + 2x \implies du = (2x + 2)\,dx; dv=cos⁡(x) dx  ⟹  v=sin⁡(x)dv = \cos(x)\,dx \implies v = \sin(x).

    2. Second pass on ∫(2x+2)sin⁡(x) dx\int (2x + 2) \sin(x)\,dx: u=2x+2  ⟹  du=2 dxu = 2x + 2 \implies du = 2\,dx; dv=sin⁡(x) dx  ⟹  v=−cos⁡(x)dv = \sin(x)\,dx \implies v = -\cos(x).

    • Result: (x2+2x−2)sin⁡(x)+(2x+2)cos⁡(x)+C(x^2 + 2x - 2) \sin(x) + (2x + 2) \cos(x) + C

  • Exercise 12: ∫t2sin⁡(βt) dt\int t^2 \sin(\beta t)\,dt

    • Requires integration by parts twice.

    • Result: −t2βcos⁡(βt)+2tβ2sin⁡(βt)+2β3cos⁡(βt)+C- \frac{t^2}{\beta} \cos(\beta t) + \frac{2t}{\beta^2} \sin(\beta t) + \frac{2}{\beta^3} \cos(\beta t) + C

  • Exercise 13: ∫cos⁡−1(x) dx\int \cos^{-1}(x)\,dx

    • Let u=cos⁡−1(x)  ⟹  du=−11−x2 dxu = \cos^{-1}(x) \implies du = -\frac{1}{\sqrt{1 - x^2}}\,dx and dv = dx \implies v = x$.\n - Result: x \cos^{-1}(x) - \sqrt{1 - x^2} + C\n\n- **Exercise 14:** \int \ln(\sqrt{x})\,dx\n - Simplify first using logarithm properties: \ln(\sqrt{x}) = \frac{1}{2} \ln(x).\n - Result: \frac{1}{2} x \ln(x) - \frac{1}{2} x + C\n\n- **Exercise 15:** \int t^4 \ln(t)\,dt\n - Let u = \ln(t) \implies du = \frac{1}{t}\,dtandanddv = t^4\,dt \implies v = \frac{1}{5} t^5$.

    • Result: 15t5ln⁡(t)−125t5+C\frac{1}{5} t^5 \ln(t) - \frac{1}{25} t^5 + C

  • Exercise 16: ∫tan⁡−1(2y) dy\int \tan^{-1}(2y)\,dy

    • Let u=tan⁡−1(2y)  ⟹  du=21+4y2 dyu = \tan^{-1}(2y) \implies du = \frac{2}{1 + 4y^2}\,dy and dv = dy \implies v = y$.\n - Result: y \tan^{-1}(2y) - \frac{1}{4} \ln(1 + 4y^2) + C\n\n- **Exercise 17:** \int t \csc^2(t)\,dt\n - Let u = t \implies du = dtandanddv = \csc^2(t)\,dt \implies v = -\cot(t).\n - Result: -t \cot(t) + \ln|\sin(t)| + C\n\n- **Exercise 18:** \int x \cosh(ax)\,dx\n - Let u = x \implies du = dxandanddv = \cosh(ax)\,dx \implies v = \frac{1}{a} \sinh(ax).\n - Result: \frac{x}{a} \sinh(ax) - \frac{1}{a^2} \cosh(ax) + C\n\n- **Exercise 19:** \int (\ln(x))^2\,dx\n - Let u = (\ln(x))^2 \implies du = \frac{2 \ln(x)}{x}\,dxandanddv = dx \implies v = x$.

    • Result: x(ln⁡(x))2−2xln⁡(x)+2x+Cx (\ln(x))^2 - 2x \ln(x) + 2x + C

  • Exercise 20: ∫z10z dz\int \frac{z}{10^z}\,dz

    • Rewrite integrand as z10−zz 10^{-z}. Let u=z  ⟹  du=dzu = z \implies du = dz and dv=10−z dz  ⟹  v=−10−zln⁡(10)dv = 10^{-z}\,dz \implies v = -\frac{10^{-z}}{\ln(10)} .

    • Result: −z10−zln⁡(10)−10−z(ln⁡(10))2+C- \frac{z 10^{-z}}{\ln(10)} - \frac{10^{-z}}{(\ln(10))^2} + C

  • Exercise 21: ∫e3xcos⁡(x) dx\int e^{3x} \cos(x)\,dx

    • Cyclic Integration by Parts: Applying integration by parts twice returns a constant multiple of the original integral II.

    • Let u=e3x,dv=cos⁡(x) dx  ⟹  I=e3xsin⁡(x)−3∫e3xsin⁡(x) dxu = e^{3x}, dv = \cos(x)\,dx \implies I = e^{3x} \sin(x) - 3 \int e^{3x} \sin(x)\,dx

    • For the second integral, let u=e3x,dv=sin⁡(x) dx  ⟹  ∫e3xsin⁡(x) dx=−e3xcos⁡(x)+3Iu = e^{3x}, dv = \sin(x)\,dx \implies \int e^{3x} \sin(x)\,dx = -e^{3x} \cos(x) + 3I

    • Solving for II:     I=e3xsin⁡(x)+3e3xcos⁡(x)−9I  ⟹  10I=e3x(sin⁡(x)+3cos⁡(x))I = e^{3x} \sin(x) + 3e^{3x} \cos(x) - 9I \implies 10I = e^{3x} (\sin(x) + 3\cos(x))

    • Result: e3x10(sin⁡(x)+3cos⁡(x))+C\frac{e^{3x}}{10} (\sin(x) + 3 \cos(x)) + C

  • Exercise 22: ∫exsin⁡(πx) dx\int e^x \sin(\pi x)\,dx

    • Cyclic Integration by Parts.

    • Result: ex1+π2(sin⁡(πx)−πcos⁡(πx))+C\frac{e^x}{1 + \pi^2} (\sin(\pi x) - \pi \cos(\pi x)) + C

  • Exercise 23: ∫e2θsin⁡(3θ) dθ\int e^{2\theta} \sin(3\theta)\,d\theta

    • Cyclic Integration by Parts.

    • Result: e2θ13(2sin⁡(3θ)−3cos⁡(3θ))+C\frac{e^{2\theta}}{13} (2 \sin(3\theta) - 3 \cos(3\theta)) + C

  • Exercise 24: ∫e−θcos⁡(2θ) dθ\int e^{-\theta} \cos(2\theta)\,d\theta

    • Cyclic Integration by Parts.

    • Result: e−θ5(−cos⁡(2θ)+2sin⁡(2θ))+C\frac{e^{-\theta}}{5} (-\cos(2\theta) + 2 \sin(2\theta)) + C

  • Exercise 25: ∫z3ez dz\int z^3 e^z\,dz

    • Tabular integration with repeated differentiation of z3z^3 down to 0.

    • Result: ez(z3−3z2+6z−6)+Ce^z (z^3 - 3z^2 + 6z - 6) + C

  • Exercise 26: ∫(arcsin⁡(x))2 dx\int (\arcsin(x))^2\,dx

    • Let u=(arcsin⁡(x))2  ⟹  du=2arcsin⁡(x)1−x2 dxu = (\arcsin(x))^2 \implies du = \frac{2 \arcsin(x)}{\sqrt{1 - x^2}}\,dx and dv = dx \implies v = x$.\n - Result: x (\arcsin(x))^2 + 2\sqrt{1 - x^2} \arcsin(x) - 2x + C\n\n- **Exercise 27:** \int (1 + x^2) e^{3x}\,dx\n - Tabular integration with u = 1 + x^2andanddv = e^{3x}\,dx$.

    • Result: e3x(13x2−29x+1127)+Ce^{3x} \left( \frac{1}{3} x^2 - \frac{2}{9} x + \frac{11}{27} \right) + C

  • Exercise 28: ∫01/2θsin⁡(3πθ) dθ\int_0^{1/2} \theta \sin(3\pi \theta)\,d\theta

    • Let u=θ,dv=sin⁡(3πθ) dθ  ⟹  du=dθ,v=−13πcos⁡(3πθ)u = \theta, dv = \sin(3\pi \theta)\,d\theta \implies du = d\theta, v = -\frac{1}{3\pi} \cos(3\pi \theta).

    • Evaluate boundary terms and remaining integral:     [−θ3πcos⁡(3πθ)]01/2+13π∫01/2cos⁡(3πθ) dθ=0+[19π2sin⁡(3πθ)]01/2=−19π2\left[ - \frac{\theta}{3\pi} \cos(3\pi \theta) \right]_0^{1/2} + \frac{1}{3\pi} \int_0^{1/2} \cos(3\pi \theta)\,d\theta = 0 + \left[ \frac{1}{9\pi^2} \sin(3\pi \theta) \right]_0^{1/2} = -\frac{1}{9\pi^2}

    • Result: −19π2-\frac{1}{9\pi^2}

  • Exercise 29: ∫01x3x dx\int_0^1 x 3^x\,dx

    • Let u=x,dv=3x dx  ⟹  du=dx,v=3xln⁡(3)u = x, dv = 3^x\,dx \implies du = dx, v = \frac{3^x}{\ln(3)}.

    • Result: 3ln⁡(3)−2(ln⁡(3))2\frac{3}{\ln(3)} - \frac{2}{(\ln(3))^2}

  • Exercise 30: ∫01xex(1+x)2 dx\int_0^1 \frac{x e^x}{(1 + x)^2}\,dx

    • Let u=xex  ⟹  du=ex(1+x) dxu = x e^x \implies du = e^x (1 + x)\,dx and dv=(1+x)−2 dx  ⟹  v=−11+xdv = (1 + x)^{-2}\,dx \implies v = -\frac{1}{1 + x}.

    • Evaluating formula:     [−xex1+x]01+∫01ex dx=−e2+(e−1)=e2−1\left[ -\frac{x e^x}{1 + x} \right]_0^1 + \int_0^1 e^x\,dx = -\frac{e}{2} + (e - 1) = \frac{e}{2} - 1

    • Result: e2−1\frac{e}{2} - 1

  • Exercise 31: ∫02ysinh⁡(y) dy\int_0^2 y \sinh(y)\,dy

    • Let u=y,dv=sinh⁡(y) dy  ⟹  du=dy,v=cosh⁡(y)u = y, dv = \sinh(y)\,dy \implies du = dy, v = \cosh(y).

    • Result: 2cosh⁡(2)−sinh⁡(2)2 \cosh(2) - \sinh(2)

  • Exercise 32: ∫12w2ln⁡(w) dw\int_1^2 w^2 \ln(w)\,dw

    • Let u = \ln(w), dv = w^2\,dw \implies du = \frac{1}{w}\,dw, v = \frac{1}{3} w^3$.\n - Result: \frac{8}{3} \ln(2) - \frac{7}{9}\n\n- **Exercise 33:** \int_1^5 \frac{\ln(R)}{R^2}\,dR\n - Let u = \ln(R), dv = R^{-2}\,dR \implies du = \frac{1}{R}\,dR, v = -R^{-1}$.

    • Result: 4−ln⁡(5)5\frac{4 - \ln(5)}{5}

  • Exercise 34: ∫02πt2sin⁡(2t) dt\int_0^{2\pi} t^2 \sin(2t)\,dt

    • Integration by parts twice over [0,2π][0, 2\pi].

    • Result: −2π2-2\pi^2

  • Exercise 35: ∫0πxsin⁡(x)cos⁡(x) dx\int_0^\pi x \sin(x) \cos(x)\,dx

    • Rewrite integrand using double-angle identity: sin⁡(x)cos⁡(x)=12sin⁡(2x)\sin(x) \cos(x) = \frac{1}{2} \sin(2x).

    • Integral becomes 12∫0πxsin⁡(2x) dx\frac{1}{2} \int_0^\pi x \sin(2x)\,dx.

    • Result: −π4-\frac{\pi}{4}

  • Exercise 36: ∫13arctan⁡(1/x) dx\int_1^{\sqrt{3}} \arctan(1/x)\,dx

    • Let u=arctan⁡(1/x)  ⟹  du=−1x2+1 dxu = \arctan(1/x) \implies du = -\frac{1}{x^2 + 1}\,dx and dv = dx \implies v = x$.\n - Result: \frac{\pi \sqrt{3}}{6} - \frac{\pi}{4} + \frac{1}{2} \ln(2)\n\n- **Exercise 37:** \int_1^5 \frac{M}{e^M}\,dM\n - Let u = M, dv = e^{-M}\,dM \implies du = dM, v = -e^{-M}.\n - Result: \frac{2}{e} - \frac{6}{e^5}\n\n- **Exercise 38:** \int_1^2 \frac{(\ln(x))^2}{x^3}\,dx\n - Let u = (\ln(x))^2, dv = x^{-3}\,dx \implies du = \frac{2 \ln(x)}{x}\,dx, v = -\frac{1}{2x^2}.\n - Result: \frac{3 - 2\ln(2) - 2(\ln(2))^2}{16}\n\n- **Exercise 39:** \int_0^{\pi/3} \sin(x) \ln(\cos(x))\,dx\n - Let u = \ln(\cos(x)) \implies du = -\tan(x)\,dxandanddv = \sin(x)\,dx \implies v = -\cos(x).\n - Result: \frac{1}{2} (\ln(2) - 1)\n\n- **Exercise 40:** \int_0^1 \frac{r^3}{\sqrt{4 + r^2}}\,dr\n - Rewrite r^3 = r^2 \cdot r.Let. Letu = r^2 \implies du = 2r\,drandanddv = \frac{r}{\sqrt{4 + r^2}}\,dr \implies v = \sqrt{4 + r^2}.\n - Result: \frac{16 - 7\sqrt{5}}{3}\n\n- **Exercise 41:** \int_0^\pi \cos(x) \sinh(x)\,dx\n - Cyclic Integration by Parts.\n - Result: -\frac{1 + \cosh(\pi)}{2}\n\n- **Exercise 42:** \int_0^t e^s \sin(t - s)\,ds\n - Integration with respect to variable s using cyclic integration by parts.\n - Result: \frac{1}{2} (e^t - \sin(t) - \cos(t))\n\n\n# Substitution Combined with Integration by Parts (Problems 43–48)\n\n- **Exercise 43:** \int e^{\sqrt{x}}\,dx\n - Substitution: Let w = \sqrt{x} \implies x = w^2 \implies dx = 2w\,dw$.

    • Integral transforms to 2 \int w e^w\,dw$.\n - Apply integration by parts (u = w, dv = e^w\,dw):):2(w e^w - e^w) + C$.

    • Substitute back: 2ex(x−1)+C2 e^{\sqrt{x}} (\sqrt{x} - 1) + C

  • Exercise 44: ∫cos⁡(ln⁡(x)) dx\int \cos(\ln(x))\,dx

    • Substitution: Let w = \ln(x) \implies x = e^w \implies dx = e^w\,dw$.\n - Integral transforms to \int e^w \cos(w)\,dw$.

    • Apply cyclic integration by parts: \frac{1}{2} e^w (\cos(w) + \sin(w)) + C$.\n - Substitute back: \frac{1}{2} x (\cos(\ln(x)) + \sin(\ln(x))) + C\n\n- **Exercise 45:** \int_{\sqrt{\pi/2}}^{\sqrt{\pi}} \theta^3 \cos(\theta^2)\,d\theta\n - Substitution: Let x = \theta^2 \implies dx = 2\theta\,d\theta$.

    • Limits change: when θ=π/2  ⟹  x=π/2\theta = \sqrt{\pi/2} \implies x = \pi/2; when \theta = \sqrt{\pi} \implies x = \pi$.\n - Integral transforms to \frac{1}{2} \int_{\pi/2}^\pi x \cos(x)\,dx$.

    • Apply integration by parts (u=x,dv=cos⁡(x) dxu = x, dv = \cos(x)\,dx).

    • Result: 12([xsin⁡(x)]π/2π−∫π/2πsin⁡(x) dx)=−π+24\frac{1}{2} \left( [x \sin(x)]_{\pi/2}^\pi - \int_{\pi/2}^\pi \sin(x)\,dx \right) = -\frac{\pi + 2}{4}

  • Exercise 46: ∫0πecos⁡(t)sin⁡(2t) dt\int_0^\pi e^{\cos(t)} \sin(2t)\,dt

    • Rewrite sin⁡(2t)=2sin⁡(t)cos⁡(t)\sin(2t) = 2 \sin(t) \cos(t).

    • Substitution: Let w = \cos(t) \implies dw = -\sin(t)\,dt$.\n - Limits change: t = 0 \implies w = 1;;t = \pi \implies w = -1$.

    • Integral transforms to 2 \int_{-1}^1 w e^w\,dw$.\n - Apply integration by parts.\n - Result: \frac{4}{e}\n\n- **Exercise 47:** \int x \ln(1 + x)\,dx\n - Substitution: Let w = 1 + x \implies x = w - 1 \implies dx = dw$.

    • Integral transforms to \int (w - 1) \ln(w)\,dw = \int w \ln(w)\,dw - \int \ln(w)\,dw$.\n - Result: \frac{x^2 - 1}{2} \ln(1 + x) - \frac{x^2}{4} + \frac{x}{2} + C\n\n- **Exercise 48:** \int \frac{\arcsin(\ln(x))}{x}\,dx\n - Substitution: Let w = \ln(x) \implies dw = \frac{1}{x}\,dx$.

    • Integral transforms to \int \arcsin(w)\,dw$.\n - Apply integration by parts (u = \arcsin(w), dv = dw).\n - Result: \ln(x) \arcsin(\ln(x)) + \sqrt{1 - (\ln(x))^2} + C\n\n\n# Indefinite Integrals and Graphical Verification (Problems 49–52)\n\n- **Instruction:** Evaluate the indefinite integral. Illustrate and verify reasonableness by graphing the function f(x)anditsantiderivativeand its antiderivativeF(x)withconstantwith constantC = 0.\n\n- **Exercise 49:** \int x e^{-2x}\,dx\n - Antiderivative (C = 0):):F(x) = -\frac{1}{4} e^{-2x} (2x + 1)\n - Function: f(x) = x e^{-2x}\n - Graphical check: F'(x) = f(x)..f(x) = 0atatx = 0,where, whereF(x)exhibitsalocalminimumatexhibits a local minimum at(0, -0.25).\n\n- **Exercise 50:** \int x^{3/2} \ln(x)\,dx\n - Antiderivative (C = 0):):F(x) = \frac{2}{25} x^{5/2} (5 \ln(x) - 2)\n - Function: f(x) = x^{3/2} \ln(x)\n\n- **Exercise 51:** \int x^3 \sqrt{1 + x^2}\,dx\n - Antiderivative (C = 0):):F(x) = \frac{1}{15} (1 + x^2)^{3/2} (3x^2 - 2)\n - Function: f(x) = x^3 \sqrt{1 + x^2}\n\n- **Exercise 52:** \int x^2 \sin(2x)\,dx\n - Antiderivative (C = 0):):F(x) = \frac{1}{4} \left( (1 - 2x^2) \cos(2x) + 2x \sin(2x) \right)\n - Function: f(x) = x^2 \sin(2x)\n\n\n# Derivation and Application of Reduction Formulas (Problems 53–62)\n\n- **Exercise 53:**\n - **Part (a):** Use the reduction formula \int \sin^n(x)\,dx = -\frac{1}{n} \sin^{n-1}(x) \cos(x) + \frac{n-1}{n} \int \sin^{n-2}(x)\,dxforforn = 2:\n    \int \sin^2(x)\,dx = -\frac{1}{2} \sin(x) \cos(x) + \frac{1}{2} \int 1\,dx = \frac{x}{2} - \frac{\sin(2x)}{4} + C\n - **Part (b):** Evaluate \int \sin^4(x)\,dxusingpart(a)andreductionforusing part (a) and reduction forn = 4:\n    \int \sin^4(x)\,dx = -\frac{1}{4} \sin^3(x) \cos(x) + \frac{3}{4} \left( \frac{x}{2} - \frac{\sin(2x)}{4} \right) + C = \frac{3}{8} x - \frac{1}{4} \sin^3(x) \cos(x) - \frac{3}{16} \sin(2x) + C\n\n- **Exercise 54:**\n - **Part (a):** Prove the reduction formula:\n    \int \cos^n(x)\,dx = \frac{1}{n} \cos^{n-1}(x) \sin(x) + \frac{n-1}{n} \int \cos^{n-2}(x)\,dx\n - *Proof:* Let u = \cos^{n-1}(x) \implies du = -(n-1)\cos^{n-2}(x)\sin(x)\,dxandanddv = \cos(x)\,dx \implies v = \sin(x).\n - Applying integration by parts:\n      \int \cos^n(x)\,dx = \cos^{n-1}(x) \sin(x) + (n-1) \int \cos^{n-2}(x) \sin^2(x)\,dx\n - Substitute \sin^2(x) = 1 - \cos^2(x):\n      \int \cos^n(x)\,dx = \cos^{n-1}(x) \sin(x) + (n-1) \int \cos^{n-2}(x)\,dx - (n-1) \int \cos^n(x)\,dx\n - Rearranging terms gives n \int \cos^n(x)\,dx = \cos^{n-1}(x) \sin(x) + (n-1) \int \cos^{n-2}(x)\,dx.Dividingby. Dividing byn completes the proof.\n - **Part (b):** Evaluate \int \cos^2(x)\,dx = \frac{x}{2} + \frac{\sin(2x)}{4} + C\n - **Part (c):** Evaluate \int \cos^4(x)\,dx = \frac{3}{8} x + \frac{1}{4} \cos^3(x) \sin(x) + \frac{3}{16} \sin(2x) + C\n\n- **Exercise 55:**\n - **Part (a):** Show that for integer n \ge 2:\n    \int_0^{\pi/2} \sin^n(x)\,dx = \frac{n-1}{n} \int_0^{\pi/2} \sin^{n-2}(x)\,dx\n - The boundary term \left[ -\frac{1}{n} \sin^{n-1}(x) \cos(x) \right]_0^{\pi/2} = 0sincesince\cos(\pi/2) = 0andand\sin(0) = 0.\n - **Part (b):** Evaluate integrals:\n - \int_0^{\pi/2} \sin^3(x)\,dx = \frac{2}{3} \int_0^{\pi/2} \sin(x)\,dx = \frac{2}{3}\n - \int_0^{\pi/2} \sin^5(x)\,dx = \frac{4}{5} \cdot \frac{2}{3} = \frac{8}{15}\n - **Part (c):** Show that for odd powers of sine (2n+1):\n    \int_0^{\pi/2} \sin^{2n+1}(x)\,dx = \frac{2 \cdot 4 \cdot 6 \cdot \cdots \cdot 2n}{3 \cdot 5 \cdot 7 \cdot \cdots \cdot (2n+1)}\n\n- **Exercise 56:** Prove that for even powers of sine (2n):\n  \int_0^{\pi/2} \sin^{2n}(x)\,dx = \frac{1 \cdot 3 \cdot 5 \cdot \cdots \cdot (2n-1)}{2 \cdot 4 \cdot 6 \cdot \cdots \cdot 2n} \frac{\pi}{2}\n\n- **Exercise 57:** Prove reduction formula for logarithm powers:\n  \int (\ln(x))^n\,dx = x (\ln(x))^n - n \int (\ln(x))^{n-1}\,dx\n - *Proof:* Let u = (\ln(x))^n \implies du = n (\ln(x))^{n-1} \frac{1}{x}\,dxandanddv = dx \implies v = x$.

  • Exercise 58: Prove reduction formula for exponential product:   ∫xnex dx=xnex−n∫xn−1ex dx\int x^n e^x\,dx = x^n e^x - n \int x^{n-1} e^x\,dx

    • Proof: Let u=xn  ⟹  du=nxn−1 dxu = x^n \implies du = n x^{n-1}\,dx and dv = e^x\,dx \implies v = e^x$.\n\n- **Exercise 59:** Prove reduction formula for tangent powers (n eq 1):\n  \int \tan^n(x)\,dx = \frac{\tan^{n-1}(x)}{n-1} - \int \tan^{n-2}(x)\,dx\n - *Proof:* Split \tan^n(x) = \tan^{n-2}(x) (\sec^2(x) - 1) = \tan^{n-2}(x) \sec^2(x) - \tan^{n-2}(x).Integratethefirsttermusingsubstitution. Integrate the first term using substitutionw = \tan(x).\n\n- **Exercise 60:** Prove reduction formula for secant powers (n eq 1):\n  \int \sec^n(x)\,dx = \frac{\tan(x) \sec^{n-2}(x)}{n-1} + \frac{n-2}{n-1} \int \sec^{n-2}(x)\,dx\n - *Proof:* Let u = \sec^{n-2}(x)andanddv = \sec^2(x)\,dx.Applyintegrationbypartsandtrigonometricidentity. Apply integration by parts and trigonometric identity\tan^2(x) = \sec^2(x) - 1$.

  • Exercise 61: Use Exercise 57 to find ∫(ln⁡(x))3 dx\int (\ln(x))^3\,dx:   ∫(ln⁡(x))3 dx=x(ln⁡(x))3−3x(ln⁡(x))2+6xln⁡(x)−6x+C\int (\ln(x))^3\,dx = x (\ln(x))^3 - 3x (\ln(x))^2 + 6x \ln(x) - 6x + C

  • Exercise 62: Use Exercise 58 to find ∫x4ex dx\int x^4 e^x\,dx:   ∫x4ex dx=ex(x4−4x3+12x2−24x+24)+C\int x^4 e^x\,dx = e^x (x^4 - 4x^3 + 12x^2 - 24x + 24) + C

Geometric Applications: Area Bounded by Curves (Problems 63–66)

  • Exercise 63: Bounded area between y=x2ln⁡(x)y = x^2 \ln(x) and y=4ln⁡(x)y = 4 \ln(x).

    • Intersection points: Set x^2 \ln(x) = 4 \ln(x) \implies (x^2 - 4) \ln(x) = 0 \implies x = 1, x = 2$.\n - On interval [1, 2],,4 \ln(x) \ge x^2 \ln(x).\n - Area integral: A = \int_1^2 (4 - x^2) \ln(x)\,dx\n - Apply integration by parts with u = \ln(x)andanddv = (4 - x^2)\,dx \implies v = 4x - \frac{x^3}{3}.\n - Result: A = \frac{16}{3} \ln(2) - \frac{29}{9}\n\n- **Exercise 64:** Bounded area between y = x^2 e^{-x}andandy = x e^{-x}.\n - Intersection points: Set x^2 e^{-x} = x e^{-x} \implies x(x - 1) = 0 \implies x = 0, x = 1$.

    • Area integral: A=∫01(x−x2)e−x dx=3e−1A = \int_0^1 (x - x^2) e^{-x}\,dx = \frac{3}{e} - 1

  • Exercise 65: Find approximate xx--coordinates of intersection and bounded area for y=arcsin⁡(12x)y = \arcsin\left(\frac{1}{2}x\right) and y=2−x2y = 2 - x^2.

    • Approximate intersection bounds: x≈−1.801x \approx -1.801 and x≈1.028x \approx 1.028

    • Area: A≈∫−1.8011.028(2−x2−arcsin⁡(12x)) dx≈4.09A \approx \int_{-1.801}^{1.028} \left( 2 - x^2 - \arcsin\left(\frac{1}{2}x\right) \right)\,dx \approx 4.09

  • Exercise 66: Find approximate xx--coordinates of intersection and bounded area for y=xln⁡(x+1)y = x \ln(x + 1) and y=3x−x2y = 3x - x^2.

    • Approximate intersection bounds: x=0x = 0 and x≈1.638x \approx 1.638

    • Area: A≈∫01.638(3x−x2−xln⁡(x+1)) dx≈1.22A \approx \int_0^{1.638} \left( 3x - x^2 - x \ln(x + 1) \right)\,dx \approx 1.22

Geometric Applications: Volumes of Solids of Revolution (Problems 67–71)

  • Exercise 67: Region bounded by y=cos⁡(πx/2)y = \cos(\pi x / 2), y=0y = 0, 0≤x≤10 \le x \le 1 rotated about the yy-axis.

    • Using cylindrical shells:     V=∫012πxcos⁡(πx/2) dx=4−8πV = \int_0^1 2\pi x \cos(\pi x / 2)\,dx = 4 - \frac{8}{\pi}

  • Exercise 68: Region bounded by y=exy = e^x, y=e−xy = e^{-x}, x=1x = 1 rotated about the yy-axis.

    • Using cylindrical shells:     V=∫012πx(ex−e−x) dx=2π([xex−ex]01−[−xe−x−e−x]01)=4πeV = \int_0^1 2\pi x (e^x - e^{-x})\,dx = 2\pi \left( [x e^x - e^x]_0^1 - [-x e^{-x} - e^{-x}]_0^1 \right) = \frac{4\pi}{e}

  • Exercise 69: Region bounded by y=e−xy = e^{-x}, y=0y = 0, x=−1x = -1, x=0x = 0 rotated about x = 1$.\n - Shell radius is 1 - x,shellheightis, shell height ise^{-x}.\n - V = \int_{-1}^0 2\pi (1 - x) e^{-x}\,dx = 2\pi e\n\n- **Exercise 70:** Region bounded by y = e^x,,x = 0,,y = 3rotatedabouttherotated about thex-axis.\n - Slicing method (washers):\n    V = \pi \int_0^{\ln(3)} (3^2 - (e^x)^2)\,dx = \pi \left[ 9x - \frac{1}{2} e^{2x} \right]0^{\ln(3)} = \pi (9 \ln(3) - 4)\n\n- **Exercise 71:** Volume generated by rotating region bounded by y = \ln(x),,y = 0,and, andx = 2:\n - **Part (a):** About the y-axis (Cylindrical Shells):\n    V = \int_1^2 2\pi x \ln(x)\,dx = \pi \left( 4 \ln(2) - \frac{3}{2} \right)\n - **Part (b):** About the x-axis (Disks):\n    V = \int_1^2 \pi (\ln(x))^2\,dx = 2\pi (\ln(2) - 1)^2\n\n\n# Advanced Calculus Applications and Functional Identities (Problems 72–78)\n\n- **Exercise 72 (Average Value of Function):** Calculate the average value of f(x) = x \sec^2(x)onon[0, \pi/4].\n - Formula: f{\text{ave}} = \frac{1}{\pi/4 - 0} \int_0^{\pi/4} x \sec^2(x)\,dx = \frac{4}{\pi} \int_0^{\pi/4} x \sec^2(x)\,dx\n - Integration by parts (u = x, dv = \sec^2(x)\,dx \implies v = \tan(x)):\n    \int_0^{\pi/4} x \sec^2(x)\,dx = [x \tan(x)]0^{\pi/4} - \int_0^{\pi/4} \tan(x)\,dx = \frac{\pi}{4} - \frac{1}{2} \ln(2)\n - Average Value: f{\text{ave}} = 1 - \frac{2 \ln(2)}{\pi}\n\n- **Exercise 73 (Optics / Fresnel Function):** The Fresnel function is defined as S(x) = \int_0^x \sin\left(\frac{1}{2}\pi t^2\right)\,dt.Find. Find\int S(x)\,dx\n - Apply integration by parts with u = S(x)andanddv = dx.\n - By the Fundamental Theorem of Calculus, S'(x) = \sin\left(\frac{1}{2}\pi x^2\right).\n - Formula: \int S(x)\,dx = x S(x) - \int x \sin\left(\frac{1}{2}\pi x^2\right)\,dx\n - Integrating remaining term via substitution w = \frac{1}{2}\pi x^2.\n - Result: x S(x) + \frac{1}{\pi} \cos\left(\frac{1}{2}\pi x^2\right) + C\n\n- **Exercise 74 (A Rocket Equation):**\n - Velocity equation: v(t) = -gt - v_e \ln\left(\frac{m - rt}{m}\right)\n - Constants: g = 9.8\,\text{m/s}^2,initialmass, initial massm = 30\,000\,\text{kg},burnrate, burn rater = 160\,\text{kg/s},exhaustvelocity, exhaust velocityv_e = 3000\,\text{m/s}.\n - Position / Height function h(t) = \int_0^t v(s)\,ds via integration by parts:\n    h(t) = - \frac{1}{2} g t^2 + v_e t + \frac{v_e (m - rt)}{r} \ln\left(\frac{m - rt}{m}\right)\n - **Part (a): Height one minute (t = 60\,\text{s}) after liftoff:**\n - m - rt = 30\,000 - 160(60) = 20\,400\,\text{kg}\n - h(60) = -\frac{1}{2}(9.8)(3600) + 3000(60) + \frac{3000(20\,400)}{160} \ln\left(\frac{20\,400}{30\,000}\right) \approx 14\,844\,\text{meters} \approx 14.8\,\text{km}\n - **Part (b): Height after burning 6000\,\text{kg} of fuel:**\n - Burn duration t = \frac{6000}{160} = 37.5\,\text{seconds},remainingmass, remaining massm - rt = 24\,000\,\text{kg}.\n - h(37.5) \approx 5195\,\text{meters} \approx 5.19\,\text{km}\n\n- **Exercise 75 (Particle Motion / Kinematics):** Straight-line motion with velocity v(t) = t^2 e^{-t}\,\text{m/s}.Distancetraveledinfirst. Distance traveled in firstt seconds:\n  s(t) = \int_0^t \tau^2 e^{-\tau}\,d\tau = \left[ -e^{-\tau} (\tau^2 + 2\tau + 2) \right]0^t = 2 - e^{-t} (t^2 + 2t + 2)\,\text{meters}\n\n- **Exercise 76 (Second Derivative Identity Proof):** Given f(0) = g(0) = 0withcontinuouswith continuousf''andandg'', show:\n  \int_0^a f(x) g''(x)\,dx = f(a) g'(a) - f'(a) g(a) + \int_0^a f''(x) g(x)\,dx\n - *Proof:* Apply integration by parts with u = f(x), dv = g''(x)\,dx \implies \int_0^a f(x) g''(x)\,dx = f(a)g'(a) - f(0)g'(0) - \int_0^a f'(x)g'(x)\,dx.Applyintegrationbypartstothesecondtermwith. Apply integration by parts to the second term withu = g'(x), dv = f'(x)\,dx.Substitutionof. Substitution off(0) = 0andandg(0) = 0 yields the identity.\n\n- **Exercise 77:** Given f(1) = 2,,f(4) = 7,,f'(1) = 5,,f'(4) = 3,evaluate, evaluate\int_1^4 x f''(x)\,dx:\n - Apply integration by parts (u = x, dv = f''(x)\,dx \implies du = dx, v = f'(x)):\n    \int_1^4 x f''(x)\,dx = [x f'(x)]_1^4 - \int_1^4 f'(x)\,dx = (4 f'(4) - 1 f'(1)) - (f(4) - f(1))\n    = (4(3) - 1(5)) - (7 - 2) = 7 - 5 = 2\n\n- **Exercise 78 (Inverse Function Integration):**\n - **Part (a):** Integration by parts identity:\n    \int f(x)\,dx = x f(x) - \int x f'(x)\,dx\n - **Part (b):** If fandandgareinversefunctions(are inverse functions (g = f^{-1}):\n    \int_a^b f(x)\,dx = b f(b) - a f(a) - \int{f(a)}^{f(b)} g(y)\,dy\n - *Proof:* Make substitution y = f(x) \implies dy = f'(x)\,dxandandx = g(y)onon\int_a^b x f'(x)\,dx.\n - **Part (c): Geometric Interpretation:** The large rectangle area b f(b)minussmallrectangleareaminus small rectangle areaa f(a)formsanL−shapedregiondecomposedintotwoorthogonalareasunderforms an L-shaped region decomposed into two orthogonal areas undery = f(x)alongthealong thex−axisand-axis andx = g(y)alongthealong they-axis.\n - **Part (d):** Evaluate \int_1^e \ln(x)\,dx using part (b):\n - Here f(x) = \ln(x) \implies g(y) = e^y.Limits:. Limits:a = 1 \implies f(1) = 0;;b = e \implies f(e) = 1$.

    • ∫1eln⁡(x) dx=eln⁡(e)−1ln⁡(1)−∫01ey dy=e−0−(e−1)=1\int_1^e \ln(x)\,dx = e \ln(e) - 1 \ln(1) - \int_0^1 e^y\,dy = e - 0 - (e - 1) = 1

Theoretical Extensions and Special Formulas (Problems 79–81)

  • Exercise 79 (Integration Formula from Quotient Rule):

    • Part (a): Derive ∫uv2 dv=−uv+∫1v du\int \frac{u}{v^2}\,dv = -\frac{u}{v} + \int \frac{1}{v}\,du

    • Proof: From Quotient Rule ddv(uv)=1vdudv−uv2\frac{d}{dv}\left(\frac{u}{v}\right) = \frac{1}{v}\frac{du}{dv} - \frac{u}{v^2}. Rearranging and integrating with respect to vv gives the formula.

    • Part (b): Evaluate ∫ln⁡(x)x2 dx\int \frac{\ln(x)}{x^2}\,dx using part (a):

    • Set u=ln⁡(x)u = \ln(x) and v = x \implies du = \frac{1}{x}\,dx$.\n - Formula gives: \int \frac{\ln(x)}{x^2}\,dx = -\frac{\ln(x)}{x} + \int \frac{1}{x^2}\,dx = -\frac{\ln(x)}{x} - \frac{1}{x} + C\n\n- **Exercise 80 (The Wallis Product Formula for \pi):**\n - Let I_n = \int_0^{\pi/2} \sin^n(x)\,dx$.

    • Part (a): Show I2n+2≤I2n+1≤I2nI_{2n+2} \le I_{2n+1} \le I_{2n}: Since 0≤sin⁡(x)≤10 \le \sin(x) \le 1 on [0,π/2][0, \pi/2], sin⁡k+1(x)≤sin⁡k(x)\sin^{k+1}(x) \le \sin^k(x).

    • Part (b): Show I2n+2I2n=2n+12n+2\frac{I_{2n+2}}{I_{2n}} = \frac{2n+1}{2n+2} using reduction formula Im=m−1mIm−2I_m = \frac{m-1}{m} I_{m-2}.

    • Part (c): Show 2n+12n+2≤I2n+1I2n≤1\frac{2n+1}{2n+2} \le \frac{I_{2n+1}}{I_{2n}} \le 1 and deduce lim⁡n→∞I2n+1I2n=1\lim_{n \to \infty} \frac{I_{2n+1}}{I_{2n}} = 1 by the Squeeze Theorem.

    • Part (d): Deduce the Wallis Product:     π2=lim⁡n→∞(21⋅23⋅43⋅45⋅65⋅67⋅⋯⋅2n2n−1⋅2n2n+1)\frac{\pi}{2} = \lim_{n \to \infty} \left( \frac{2}{1} \cdot \frac{2}{3} \cdot \frac{4}{3} \cdot \frac{4}{5} \cdot \frac{6}{5} \cdot \frac{6}{7} \cdot \cdots \cdot \frac{2n}{2n-1} \cdot \frac{2n}{2n+1} \right)     π2=21⋅23⋅43⋅45⋅65⋅67⋅⋯\frac{\pi}{2} = \frac{2}{1} \cdot \frac{2}{3} \cdot \frac{4}{3} \cdot \frac{4}{5} \cdot \frac{6}{5} \cdot \frac{6}{7} \cdot \cdots

    • Part (e): Ratio of width to height for nested rectangles:          

      Nested Rectangles Diagram

          

    • Starting with unit square (area 1), attach rectangles of area 1 alternately beside or on top.

    • Sequence of ratios of width to height reproduces the partial products of the Wallis product.

    • Limit of ratio of width to height as n→∞n \to \infty is π2\frac{\pi}{2}.

  • Exercise 81 (Proof of Shell Method Volume via Integration by Parts):      

    Solid of Revolution Volume Region
    • Slicing formula for solid rotated about yy-axis:     V=πb2d−πa2c−∫cdπ[g(y)]2 dyV = \pi b^2 d - \pi a^2 c - \int_c^d \pi [g(y)]^2\,dy

    • Substitution y=f(x)  ⟹  dy=f′(x) dxy = f(x) \implies dy = f'(x)\,dx and g(y)=xg(y) = x transforms integral to:     ∫cdπ[g(y)]2 dy=∫abπx2f′(x) dx\int_c^d \pi [g(y)]^2\,dy = \int_a^b \pi x^2 f'(x)\,dx

    • Apply integration by parts to ∫abx2f′(x) dx\int_a^b x^2 f'(x)\,dx (u=x2,dv=f′(x) dx  ⟹  v=f(x)u = x^2, dv = f'(x)\,dx \implies v = f(x)):     ∫abx2f′(x) dx=[x2f(x)]ab−∫ab2xf(x) dx=b2d−a2c−∫ab2xf(x) dx\int_a^b x^2 f'(x)\,dx = [x^2 f(x)]_a^b - \int_a^b 2x f(x)\,dx = b^2 d - a^2 c - \int_a^b 2x f(x)\,dx

    • Substituting back into formula for VV:     V=πb2d−πa2c−π(b2d−a2c−∫ab2xf(x) dx)=∫ab2πxf(x) dxV = \pi b^2 d - \pi a^2 c - \pi \left( b^2 d - a^2 c - \int_a^b 2x f(x)\,dx \right) = \int_a^b 2\pi x f(x)\,dx

    • This proves the Cylindrical Shells volume formula using horizontal slicing and integration by parts.