Advanced Integration Techniques - IB Mathematics Analysis and Approaches

  1. Using the substitution u=cos⁡θu = \cos \theta, which of the following integrals is equivalent to ∫sin⁡3θ dθ\int \sin^3 \theta \, d\theta?
    Answer: ∫(u2−1) du\int (u^2-1) \, du To use the substitution u=cos⁡θu = \cos \theta, we first need to express the integrand in terms of cos⁡θ\cos \theta and a single sin⁡θ\sin \theta. We write sin⁡3θ=sin⁡2θ⋅sin⁡θ=(1−cos⁡2θ)sin⁡θ\sin^3 \theta = \sin^2 \theta \cdot \sin \theta = (1-\cos^2 \theta) \sin \theta. So the integral is ∫(1−cos⁡2θ)sin⁡θ dθ\int (1-\cos^2 \theta) \sin \theta \, d\theta. Now, let u=cos⁡θu = \cos \theta. Then du=−sin⁡θ dθdu = -\sin \theta \, d\theta, which means sin⁡θ dθ=−du\sin \theta \, d\theta = -du. Substituting these into the integral gives: ∫(1−u2)(−du)=∫(u2−1) du \int (1-u^2) (-du) = \int (u^2-1) \, du Distractor A is a very common error where the negative sign from du=−sin⁡θ dθdu = -\sin \theta \, d\theta is forgotten. Distractor C arises from incorrectly substituting u2u^2 for sin⁡2θ\sin^2 \theta. Distractor D would arise from an incorrect substitution setup.
  2. Find the integral ∫1x+xdx\int \frac{1}{x + \sqrt{x}} dx.
    Answer: 2ln⁡(x+1)+C2 \ln(\sqrt{x}+1) + C This integral can be solved with the substitution u=xu = \sqrt{x}. This implies u2=xu^2 = x and 2u du=dx2u \, du = dx. Substituting into the integral: ∫1x+xdx=∫1u2+u(2u du) \int \frac{1}{x + \sqrt{x}} dx = \int \frac{1}{u^2 + u} (2u \, du) Factor the denominator and simplify: ∫2uu(u+1)du=∫2u+1du \int \frac{2u}{u(u+1)} du = \int \frac{2}{u+1} du This is a standard logarithmic integral: 2ln⁡∣u+1∣+C 2 \ln|u+1| + C Substituting back u=xu = \sqrt{x}: 2ln⁡(x+1)+C 2 \ln(\sqrt{x}+1) + C (Absolute value is not necessary since x≥0\sqrt{x} \ge 0, so x+1>0\sqrt{x}+1 > 0). Distractor A is a naive guess, as if ∫1/f(x)dx=ln⁡∣f(x)∣\int 1/f(x) dx = \ln|f(x)| which is generally untrue. Distractor B results from forgetting the 2u2u factor in dx=2u dudx = 2u \, du, which leads to integrating 1u(u+1)\frac{1}{u(u+1)}. Distractor D results from an incorrect integration of 2u+1\frac{2}{u+1}.
  3. Find ∫xx−2 dx\int x \sqrt{x-2} \, dx.
    Answer: 215(x−2)3/2(3x+4)+C\frac{2}{15}(x-2)^{3/2}(3x+4)+C This integral is best solved using substitution. Let u=x−2u = x-2, which means x=u+2x = u+2 and du=dxdu = dx. The integral becomes: ∫(u+2)u du=∫(u3/2+2u1/2) du \int (u+2)\sqrt{u} \, du = \int (u^{3/2} + 2u^{1/2}) \, du Now, integrate with respect to uu: u5/25/2+2u3/23/2+C=25u5/2+43u3/2+C \frac{u^{5/2}}{5/2} + 2\frac{u^{3/2}}{3/2} + C = \frac{2}{5}u^{5/2} + \frac{4}{3}u^{3/2} + C Substitute back u=x−2u=x-2: 25(x−2)5/2+43(x−2)3/2+C \frac{2}{5}(x-2)^{5/2} + \frac{4}{3}(x-2)^{3/2} + C To match the answer choices, factor out 215(x−2)3/2\frac{2}{15}(x-2)^{3/2}: 215(x−2)3/2[3(x−2)+10]+C=215(x−2)3/2(3x−6+10)+C=215(x−2)3/2(3x+4)+C \frac{2}{15}(x-2)^{3/2} [3(x-2) + 10] + C = \frac{2}{15}(x-2)^{3/2} (3x-6+10) + C = \frac{2}{15}(x-2)^{3/2}(3x+4)+C Distractor A ignores the factor of xx in the integrand. Distractor B only integrates the first term that would arise from the substitution, ∫uu du\int u \sqrt{u} \, du. Distractor C comes from an incorrect substitution x=u−2x=u-2 instead of x=u+2x=u+2, leading to a sign error.
  4. Determine the value of ∫1eln⁡xx2dx\int_{1}^{e} \frac{\ln x}{x^2} dx.
    Answer: 1−2e1 - \frac{2}{e} We use integration by parts. Let u=ln⁡xu = \ln x and dv=1x2dx=x−2dxdv = \frac{1}{x^2} dx = x^{-2} dx. Then du=1xdxdu = \frac{1}{x} dx and v=−x−1=−1xv = -x^{-1} = -\frac{1}{x}. Applying the formula ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du: ∫1eln⁡xx2dx=[−ln⁡xx]1e−∫1e(−1x)1xdx \int_{1}^{e} \frac{\ln x}{x^2} dx = \left[-\frac{\ln x}{x}\right]_{1}^{e} - \int_{1}^{e} \left(-\frac{1}{x}\right) \frac{1}{x} dx =[−ln⁡xx]1e+∫1e1x2dx = \left[-\frac{\ln x}{x}\right]_{1}^{e} + \int_{1}^{e} \frac{1}{x^2} dx =[−ln⁡xx−1x]1e = \left[-\frac{\ln x}{x} - \frac{1}{x}\right]_{1}^{e} Now evaluate at the limits: =(−ln⁡ee−1e)−(−ln⁡11−11) = \left(-\frac{\ln e}{e} - \frac{1}{e}\right) - \left(-\frac{\ln 1}{1} - \frac{1}{1}\right) =(−1e−1e)−(0−1) = \left(-\frac{1}{e} - \frac{1}{e}\right) - \left(0 - 1\right) =−2e−(−1)=1−2e = -\frac{2}{e} - (-1) = 1 - \frac{2}{e} Distractor B comes from an error in the sign when integrating dvdv, taking v=1/xv = 1/x. Distractor D results from incorrectly evaluating ln⁡1=1\ln 1 = 1 instead of 0. Distractor A arises from a combination of sign errors.
  5. Which of the following is an expression for ∫sin⁡(ln⁡x) dx\int \sin(\ln x) \, dx?
    Answer: x2(sin⁡(ln⁡x)−cos⁡(ln⁡x))+C\frac{x}{2}(\sin(\ln x) - \cos(\ln x)) + C This problem can be solved with integration by parts, or substitution followed by parts. Using parts directly is efficient. Let I=∫sin⁡(ln⁡x)dxI = \int \sin(\ln x) dx. Let u=sin⁡(ln⁡x)u = \sin(\ln x) and dv=dxdv = dx. Then du=cos⁡(ln⁡x)⋅1xdxdu = \cos(\ln x) \cdot \frac{1}{x} dx and v=xv = x. I=xsin⁡(ln⁡x)−∫x⋅cos⁡(ln⁡x)1xdx=xsin⁡(ln⁡x)−∫cos⁡(ln⁡x)dx I = x \sin(\ln x) - \int x \cdot \cos(\ln x) \frac{1}{x} dx = x \sin(\ln x) - \int \cos(\ln x) dx Apply parts to the new integral. Let u=cos⁡(ln⁡x)u = \cos(\ln x) and dv=dxdv = dx. Then du=−sin⁡(ln⁡x)⋅1xdxdu = -\sin(\ln x) \cdot \frac{1}{x} dx and v=xv = x. ∫cos⁡(ln⁡x)dx=xcos⁡(ln⁡x)−∫x(−sin⁡(ln⁡x)1x)dx=xcos⁡(ln⁡x)+∫sin⁡(ln⁡x)dx=xcos⁡(ln⁡x)+I \int \cos(\ln x) dx = x \cos(\ln x) - \int x \left(-\sin(\ln x) \frac{1}{x}\right) dx = x \cos(\ln x) + \int \sin(\ln x) dx = x \cos(\ln x) + I Substitute this back into the equation for II: I=xsin⁡(ln⁡x)−(xcos⁡(ln⁡x)+I) I = x \sin(\ln x) - (x \cos(\ln x) + I) I=xsin⁡(ln⁡x)−xcos⁡(ln⁡x)−I I = x \sin(\ln x) - x \cos(\ln x) - I 2I=x(sin⁡(ln⁡x)−cos⁡(ln⁡x)) 2I = x(\sin(\ln x) - \cos(\ln x)) I=x2(sin⁡(ln⁡x)−cos⁡(ln⁡x))+C I = \frac{x}{2}(\sin(\ln x) - \cos(\ln x)) + C Distractor A results from forgetting to divide by 2 when solving for II. Distractor B has a sign error, corresponding to the result for ∫cos⁡(ln⁡x)dx\int \cos(\ln x) dx. Distractor C misses the factor of xx that arises from the integration.
  6. What is the value of the integral ∫1e2(ln⁡x)2xdx\int_{1}^{e^2} \frac{(\ln x)^2}{x} dx?
    Answer: 83\frac{8}{3} We use substitution. Let u=ln⁡xu = \ln x. Then du=1xdxdu = \frac{1}{x} dx. We must change the limits of integration. When x=1x=1, u=ln⁡1=0u=\ln 1=0. When x=e2x=e^2, u=ln⁡(e2)=2u=\ln(e^2)=2. The integral becomes: ∫02u2du \int_{0}^{2} u^2 du Now, we integrate with respect to uu: [u33]02=233−033=83 \left[\frac{u^3}{3}\right]_{0}^{2} = \frac{2^3}{3} - \frac{0^3}{3} = \frac{8}{3} Distractor A results from integrating uu instead of u2u^2, giving u2/2u^2/2. Distractor C comes from integrating u2u^2 to u3u^3 but forgetting to divide by 3. Distractor D results from failing to perform the substitution correctly.
  7. Let f(x)f(x) be a differentiable function. Which of the following is equivalent to ∫xf′′(x)dx\int x f''(x) dx?
    Answer: xf′(x)−f(x)+Cx f'(x) - f(x) + C We use integration by parts with u=xu=x and dv=f′′(x)dxdv=f''(x)dx. From these choices, we have: du=dxdu = dx v=∫f′′(x)dx=f′(x)v = \int f''(x)dx = f'(x) Applying the integration by parts formula, ∫u dv=uv−∫v du\int u\,dv = uv - \int v\,du: ∫xf′′(x)dx=xf′(x)−∫f′(x)dx \int x f''(x) dx = x f'(x) - \int f'(x) dx Since ∫f′(x)dx=f(x)+C1\int f'(x) dx = f(x) + C_1, the expression becomes: xf′(x)−(f(x)+C1)=xf′(x)−f(x)+C x f'(x) - (f(x) + C_1) = x f'(x) - f(x) + C where C=−C1C = -C_1 is the constant of integration. Distractor B comes from a sign error in the integration by parts formula (uv+∫v duuv + \int v\,du). Distractor C results from an incorrect application of integration by parts. Distractor D arises from incorrectly integrating f′′(x)f''(x) to get f(x)f(x).
  8. To evaluate the integral ∫cos⁡x4+sin⁡2xdx\int \frac{\cos x}{4 + \sin^2 x} dx, a substitution is made. If the resulting integral is ∫14+u2du\int \frac{1}{4+u^2} du, what was the substitution for uu?
    Answer: u=sin⁡xu = \sin x Let's test the substitution u=sin⁡xu = \sin x. The derivative is dudx=cos⁡x\frac{du}{dx} = \cos x, so du=cos⁡xdxdu = \cos x dx. The denominator becomes 4+(sin⁡x)2=4+u24 + (\sin x)^2 = 4 + u^2. The numerator, cos⁡xdx\cos x dx, becomes dudu. Substituting these into the original integral gives: ∫cos⁡x4+sin⁡2xdx=∫14+u2du \int \frac{\cos x}{4 + \sin^2 x} dx = \int \frac{1}{4+u^2} du This matches the integral given in the question. Therefore, the correct substitution is u=sin⁡xu = \sin x. The other options lead to more complicated or incorrect integrals. For example, if u=cos⁡xu = \cos x, the numerator becomes uu but sin⁡2x=1−u2\sin^2 x = 1-u^2 and dx=−du/sin⁡xdx = -du/\sin x, which does not simplify correctly.
  9. Let g(x)=∫1x2sin⁡(t)tdtg(x) = \int_{1}^{x^2} \frac{\sin(t)}{\sqrt{t}} dt. What is the value of g′(π)g'(\sqrt{\pi})?
    Answer: 00 This question requires the application of the Fundamental Theorem of Calculus Part 2, combined with the chain rule. If F(x)=∫ah(x)f(t)dtF(x) = \int_{a}^{h(x)} f(t) dt, then F′(x)=f(h(x))⋅h′(x)F'(x) = f(h(x)) \cdot h'(x). In this case, f(t)=sin⁡(t)tf(t) = \frac{\sin(t)}{\sqrt{t}} and the upper limit is h(x)=x2h(x) = x^2. The derivative of the upper limit is h′(x)=2xh'(x) = 2x. So, g′(x)=sin⁡(x2)x2⋅(2x)g'(x) = \frac{\sin(x^2)}{\sqrt{x^2}} \cdot (2x). For x>0x>0, x2=x\sqrt{x^2}=x, so g′(x)=sin⁡(x2)x⋅(2x)=2sin⁡(x2)g'(x) = \frac{\sin(x^2)}{x} \cdot (2x) = 2\sin(x^2). We need to find g′(π)g'(\sqrt{\pi}): g′(π)=2sin⁡((π)2)=2sin⁡(π)=2⋅0=0 g'(\sqrt{\pi}) = 2\sin((\sqrt{\pi})^2) = 2\sin(\pi) = 2 \cdot 0 = 0 Distractor A results from miscalculation or errors in applying the chain rule. Distractor D might arise from forgetting the sin⁡\sin function and evaluating 22 at x=πx=\sqrt{\pi}.
  10. The integral ∫x31−x2dx\int \frac{x^3}{\sqrt{1-x^2}} dx can be solved using the substitution x=sin⁡θx=\sin\theta. Which of the following is the resulting integral in terms of θ\theta?
    Answer: ∫sin⁡3θ dθ\int \sin^3\theta \, d\theta Let x=sin⁡θx = \sin\theta. Then dx=cos⁡θ dθdx = \cos\theta \, d\theta. The numerator is x3=sin⁡3θx^3 = \sin^3\theta. The denominator is 1−x2=1−sin⁡2θ=cos⁡2θ=cos⁡θ\sqrt{1-x^2} = \sqrt{1-\sin^2\theta} = \sqrt{\cos^2\theta} = \cos\theta (assuming cos⁡θ>0\cos\theta > 0, which is standard for this substitution). Substituting these into the integral: ∫sin⁡3θcos⁡θ(cos⁡θ dθ) \int \frac{\sin^3\theta}{\cos\theta} (\cos\theta \, d\theta) The cos⁡θ\cos\theta terms cancel out, leaving: ∫sin⁡3θ dθ \int \sin^3\theta \, d\theta Distractor B results from forgetting to substitute for dxdx. Distractor C and D come from incorrect algebraic simplification after substitution.
  11. Find ∫(x2+1)ln⁡x dx\int (x^2 + 1) \ln x \, dx.
    Answer: (x33+x)ln⁡x−x39−x+C\left(\frac{x^3}{3} + x\right)\ln x - \frac{x^3}{9} - x + C We use integration by parts, ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du. Following the LIATE/LATE principle, we choose u=ln⁡xu = \ln x and dv=(x2+1)dxdv = (x^2 + 1) dx. Then du=1xdxdu = \frac{1}{x} dx and v=x33+xv = \frac{x^3}{3} + x. ∫(x2+1)ln⁡x dx=(x33+x)ln⁡x−∫(x33+x)1xdx \int (x^2 + 1) \ln x \, dx = \left(\frac{x^3}{3} + x\right)\ln x - \int \left(\frac{x^3}{3} + x\right) \frac{1}{x} dx =(x33+x)ln⁡x−∫(x23+1)dx = \left(\frac{x^3}{3} + x\right)\ln x - \int \left(\frac{x^2}{3} + 1\right) dx =(x33+x)ln⁡x−(x39+x)+C = \left(\frac{x^3}{3} + x\right)\ln x - \left(\frac{x^3}{9} + x\right) + C =(x33+x)ln⁡x−x39−x+C = \left(\frac{x^3}{3} + x\right)\ln x - \frac{x^3}{9} - x + C Distractor A comes from a power rule error when integrating x23\frac{x^2}{3}. Distractor B results from a sign error in the integration by parts formula (using uv+∫v duuv + \int v \, du). Distractor D incorrectly differentiates x2+1x^2+1 instead of integrating it.
  12. Evaluate ∫x2sin⁡x dx\int x^2 \sin x \, dx.
    Answer: −x2cos⁡x+2xsin⁡x+2cos⁡x+C-x^2 \cos x + 2x \sin x + 2\cos x + C This requires repeated integration by parts. Let's use the tabular method for efficiency. Let uu-column be for differentiation and dvdv-column for integration.
    DifferentiateIntegrate
    x2x^2sin⁡x\sin x
    2x2x−cos⁡x-\cos x
    22−sin⁡x-\sin x
    00cos⁡x\cos x
    Multiply diagonally with alternating signs (+, -, +): 1. +(x2)(−cos⁡x)=−x2cos⁡x+(x^2)(-\cos x) = -x^2 \cos x 2. −(2x)(−sin⁡x)=+2xsin⁡x-(2x)(-\sin x) = +2x \sin x 3. +(2)(cos⁡x)=+2cos⁡x+(2)(\cos x) = +2\cos x Summing these terms gives the integral: ∫x2sin⁡x dx=−x2cos⁡x+2xsin⁡x+2cos⁡x+C \int x^2 \sin x \, dx = -x^2 \cos x + 2x \sin x + 2\cos x + C Distractors A, B, and D are variations with incorrect signs, which commonly arise from errors in the alternating signs of the tabular method or in the integrals/derivatives of sin and cos.
  13. Calculate the exact value of ∫0ln⁡2ex1+e2xdx\int_{0}^{\ln 2} \frac{e^x}{1+e^{2x}} dx.
    Answer: arctan⁡(2)−π4\arctan(2) - \frac{\pi}{4} We use substitution. Let u=exu = e^x. Then du=exdxdu = e^x dx. We must also change the limits of integration. When x=0x=0, u=e0=1u=e^0=1. When x=ln⁡2x=\ln 2, u=eln⁡2=2u=e^{\ln 2}=2. The integral becomes: ∫1211+u2du \int_{1}^{2} \frac{1}{1+u^2} du This is a standard integral: [arctan⁡(u)]12=arctan⁡(2)−arctan⁡(1) \left[\arctan(u)\right]_{1}^{2} = \arctan(2) - \arctan(1) Since arctan⁡(1)=π4\arctan(1) = \frac{\pi}{4}, the result is arctan⁡(2)−π4\arctan(2) - \frac{\pi}{4}. Distractor A results from incorrectly integrating 11+u2\frac{1}{1+u^2} to get ln⁡(1+u2)\ln(1+u^2). Distractor B is a common error where the limits of integration are not changed after the substitution. Distractor D results from forgetting to evaluate the integral at the lower limit.
  14. Find the exact value of ∫01xe2xdx\int_{0}^{1} x e^{2x} dx.
    Answer: e2+14\frac{e^2+1}{4} This integral requires integration by parts, using the formula ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du. Let u=xu = x and dv=e2xdxdv = e^{2x} dx. Then du=dxdu = dx and v=12e2xv = \frac{1}{2}e^{2x}. Applying the formula for the definite integral: ∫01xe2xdx=[x⋅12e2x]01−∫0112e2xdx \int_{0}^{1} x e^{2x} dx = \left[x \cdot \frac{1}{2}e^{2x}\right]_{0}^{1} - \int_{0}^{1} \frac{1}{2}e^{2x} dx =[12xe2x]01−[14e2x]01 = \left[\frac{1}{2}xe^{2x}\right]_{0}^{1} - \left[\frac{1}{4}e^{2x}\right]_{0}^{1} =(12(1)e2−12(0)e0)−(14e2−14e0) = \left(\frac{1}{2}(1)e^{2} - \frac{1}{2}(0)e^{0}\right) - \left(\frac{1}{4}e^{2} - \frac{1}{4}e^{0}\right) =12e2−(14e2−14) = \frac{1}{2}e^{2} - \left(\frac{1}{4}e^{2} - \frac{1}{4}\right) =12e2−14e2+14=14e2+14=e2+14 = \frac{1}{2}e^{2} - \frac{1}{4}e^{2} + \frac{1}{4} = \frac{1}{4}e^{2} + \frac{1}{4} = \frac{e^2+1}{4} Distractor A results from a sign error in the formula, calculating uv−(−∫v du)uv - (-\int v\,du) which becomes uv+∫v duuv+\int v\,du but then making another sign error in evaluation. Distractor C occurs if one forgets that e0=1e^0=1 and treats the lower bound evaluation as zero. Distractor D results from forgetting the factor of 1/21/2 when integrating e2xe^{2x} the first time, i.e., incorrectly taking v=e2xv=e^{2x}.
  15. Find ∫arctan⁡(x)dx\int \arctan(x) dx.
    Answer: xarctan⁡(x)−12ln⁡(1+x2)+Cx \arctan(x) - \frac{1}{2} \ln(1+x^2) + C This is a standard integration by parts problem where dv=dxdv=dx. Let u=arctan⁡(x)u = \arctan(x) and dv=dxdv = dx. Then du=11+x2dxdu = \frac{1}{1+x^2} dx and v=xv = x. Using the formula ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du: ∫arctan⁡(x)dx=xarctan⁡(x)−∫x⋅11+x2dx=xarctan⁡(x)−∫x1+x2dx \int \arctan(x) dx = x \arctan(x) - \int x \cdot \frac{1}{1+x^2} dx = x \arctan(x) - \int \frac{x}{1+x^2} dx To evaluate the remaining integral, we use substitution. Let w=1+x2w = 1+x^2, so dw=2xdxdw = 2x dx, or xdx=12dwx dx = \frac{1}{2} dw. ∫x1+x2dx=∫1w(12dw)=12ln⁡∣w∣+C=12ln⁡(1+x2)+C \int \frac{x}{1+x^2} dx = \int \frac{1}{w} \left(\frac{1}{2} dw\right) = \frac{1}{2} \ln|w| + C = \frac{1}{2} \ln(1+x^2) + C (Absolute value is not needed as 1+x2>01+x^2 > 0). Combining the results gives: xarctan⁡(x)−12ln⁡(1+x2)+C x \arctan(x) - \frac{1}{2} \ln(1+x^2) + C Distractor A results from forgetting the factor of 1/21/2 from the substitution. Distractor B has a sign error from the integration by parts formula. Distractor C arises from incorrectly remembering the derivative of arctan⁡(x)\arctan(x) as the derivative of arcsin⁡(x)\arcsin(x).
  16. Given that ∫a2a1xln⁡xdx=ln⁡3\int_{a}^{2a} \frac{1}{x \ln x} dx = \ln 3 for a>1a>1, find the value of aa.
    Answer: 2\sqrt{2} To solve the integral ∫1xln⁡xdx\int \frac{1}{x \ln x} dx, we use the substitution u=ln⁡xu = \ln x. This gives du=1xdxdu = \frac{1}{x} dx. We must also change the limits of integration. When x=ax=a, u=ln⁡au=\ln a. When x=2ax=2a, u=ln⁡(2a)u=\ln(2a). The integral becomes: ∫ln⁡aln⁡(2a)1udu=[ln⁡∣u∣]ln⁡aln⁡(2a) \int_{\ln a}^{\ln(2a)} \frac{1}{u} du = [\ln|u|]_{\ln a}^{\ln(2a)} Since a>1a>1, ln⁡a>0\ln a > 0 and ln⁡(2a)>0\ln(2a) > 0. ln⁡(ln⁡(2a))−ln⁡(ln⁡a)=ln⁡(ln⁡(2a)ln⁡a) \ln(\ln(2a)) - \ln(\ln a) = \ln\left(\frac{\ln(2a)}{\ln a}\right) We are given that this value is ln⁡3\ln 3. Therefore: ln⁡(2a)ln⁡a=3 \frac{\ln(2a)}{\ln a} = 3 ln⁡(2a)=3ln⁡a \ln(2a) = 3 \ln a Using logarithm properties, 3ln⁡a=ln⁡(a3)3 \ln a = \ln(a^3). ln⁡(2a)=ln⁡(a3) \ln(2a) = \ln(a^3) 2a=a3 2a = a^3 Since a>1a>1, we can divide by aa: 2=a2  ⟹  a=2 2 = a^2 \implies a = \sqrt{2} Distractor C, a=2a=2, might result from the error ln⁡(2a)=ln⁡(2)+ln⁡(a)\ln(2a) = \ln(2) + \ln(a), leading to ln⁡(2)+ln⁡(a)=3ln⁡(a)\ln(2)+\ln(a) = 3\ln(a) or ln⁡(2)=2ln⁡(a)=ln⁡(a2)\ln(2) = 2\ln(a) = \ln(a^2), so a2=2a^2=2. This logic is correct. What error leads to a=2a=2? Perhaps ln⁡(2a)ln⁡a=ln⁡(2)\frac{\ln(2a)}{\ln a} = \ln(2)? No. Perhaps 2aa=3\frac{2a}{a}=3? No. An error in log rules like ln⁡(2a)=2ln⁡(a)\ln(2a) = 2\ln(a) might lead to 2ln⁡(a)=3ln⁡(a)2\ln(a)=3\ln(a), which means ln⁡(a)=0\ln(a)=0, so a=1a=1, not an option. Distractor B may come from setting the expression equal to 3 instead of ln⁡3\ln 3. Distractor C, a=2, is a common guess.
  17. Which substitution would be most effective to find the integral ∫1ex+e−xdx\int \frac{1}{e^x + e^{-x}} dx?
    Answer: u=exu = e^x First, algebraically manipulate the integrand: ∫1ex+e−xdx=∫1ex+1exdx=∫1e2x+1exdx=∫exe2x+1dx \int \frac{1}{e^x + e^{-x}} dx = \int \frac{1}{e^x + \frac{1}{e^x}} dx = \int \frac{1}{\frac{e^{2x}+1}{e^x}} dx = \int \frac{e^x}{e^{2x}+1} dx Now, the integral is in a form suitable for substitution. Let u=exu = e^x. Then du=exdxdu = e^x dx and e2x=(ex)2=u2e^{2x} = (e^x)^2 = u^2. The integral becomes: ∫1u2+1du \int \frac{1}{u^2+1} du This is a standard integral (arctan⁡(u)+C\arctan(u) + C), so the substitution u=exu=e^x is effective. Distractor A, u=ex+e−xu = e^x + e^{-x}, leads to du=(ex−e−x)dxdu = (e^x - e^{-x})dx, which does not simplify the integral. Distractor C, u=e−xu=e^{-x}, is also workable but u=exu=e^x is more direct. Distractor D is not a substitution.
  18. The value of ∫0π/2xcos⁡(x)dx\int_{0}^{\pi/2} x \cos(x) dx is:
    Answer: π2−1\frac{\pi}{2} - 1 We use integration by parts. Let u=xu=x and dv=cos⁡(x)dxdv = \cos(x) dx. Then du=dxdu=dx and v=sin⁡(x)v=\sin(x). ∫0π/2xcos⁡(x)dx=[xsin⁡(x)]0π/2−∫0π/2sin⁡(x)dx \int_{0}^{\pi/2} x \cos(x) dx = [x \sin(x)]_{0}^{\pi/2} - \int_{0}^{\pi/2} \sin(x) dx =[xsin⁡(x)−(−cos⁡(x))]0π/2=[xsin⁡(x)+cos⁡(x)]0π/2 = [x \sin(x) - (-\cos(x))]_{0}^{\pi/2} = [x \sin(x) + \cos(x)]_{0}^{\pi/2} Now, evaluate at the limits: (π2sin⁡(π2)+cos⁡(π2))−(0⋅sin⁡(0)+cos⁡(0)) \left(\frac{\pi}{2} \sin\left(\frac{\pi}{2}\right) + \cos\left(\frac{\pi}{2}\right)\right) - (0 \cdot \sin(0) + \cos(0)) =(π2⋅1+0)−(0+1) = \left(\frac{\pi}{2} \cdot 1 + 0\right) - (0 + 1) =π2−1 = \frac{\pi}{2} - 1 Distractor A results from calculation errors, possibly cos⁡(0)=0\cos(0)=0. Distractor B results from ignoring the second term ∫vdu\int v du. Distractor D comes from a sign error when integrating sin⁡(x)\sin(x), i.e., ∫sin⁡(x)dx=cos⁡(x)\int \sin(x) dx = \cos(x).
  19. Determine the value of AA.
    Answer: 15\frac{1}{5} We use integration by parts, ∫u dv=uv−∫v du\int u \, dv = uv - \int v \, du. Let u=e2xu = e^{2x} and dv=cos⁡x dxdv = \cos x \, dx. Then du=2e2x dxdu = 2e^{2x} \, dx and v=sin⁡xv = \sin x. I=e2xsin⁡x−∫2e2xsin⁡x dx I = e^{2x} \sin x - \int 2e^{2x} \sin x \, dx Apply integration by parts again to the new integral. Let u=2e2xu = 2e^{2x} and dv=sin⁡x dxdv = \sin x \, dx. Then du=4e2x dxdu = 4e^{2x} \, dx and v=−cos⁡xv = -\cos x. I=e2xsin⁡x−(−2e2xcos⁡x−∫−4e2xcos⁡x dx) I = e^{2x} \sin x - \left( -2e^{2x} \cos x - \int -4e^{2x} \cos x \, dx \right) I=e2xsin⁡x+2e2xcos⁡x−4∫e2xcos⁡x dx I = e^{2x} \sin x + 2e^{2x} \cos x - 4 \int e^{2x} \cos x \, dx Since I=∫e2xcos⁡x dxI = \int e^{2x} \cos x \, dx, we have: I=e2xsin⁡x+2e2xcos⁡x−4I I = e^{2x} \sin x + 2e^{2x} \cos x - 4I 5I=e2x(sin⁡x+2cos⁡x) 5I = e^{2x}(\sin x + 2\cos x) I=15e2x(sin⁡x+2cos⁡x)+C=e2x(15sin⁡x+25cos⁡x)+C I = \frac{1}{5}e^{2x}(\sin x + 2\cos x) + C = e^{2x}\left(\frac{1}{5}\sin x + \frac{2}{5}\cos x\right) + C Comparing this to e2x(Asin⁡x+Bcos⁡x)+Ce^{2x}(A \sin x + B \cos x) + C, we find A=15A = \frac{1}{5}. Distractor D is the value of BB. Distractor A results from a sign error in the integration by parts formula. Distractor C arises from algebraic mistakes when solving for II.

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