Taylor Polynomial Approximations - Calculus 2

  1. The third-degree Taylor polynomial for f(x)=e2xf(x) = e^{2x} centered at x=0x = 0 is used to approximate f(0.1)f(0.1). If the actual value is e0.2≈1.2214e^{0.2} \approx 1.2214, what is the absolute error in this approximation?
    Answer: Approximately 0.0014 The third-degree Taylor polynomial for e2xe^{2x} at x=0x = 0 is P3(x)=1+2x+(2x)22!+(2x)33!=1+2x+2x2+4x33P_3(x) = 1 + 2x + \frac{(2x)^2}{2!} + \frac{(2x)^3}{3!} = 1 + 2x + 2x^2 + \frac{4x^3}{3}. At x=0.1x = 0.1: P3(0.1)=1+0.2+0.02+0.0043≈1.2200P_3(0.1) = 1 + 0.2 + 0.02 + \frac{0.004}{3} \approx 1.2200. The absolute error is ∣1.2214−1.2200∣≈0.0014|1.2214 - 1.2200| \approx 0.0014. Choice A uses only terms up to x2x^2, choice C incorrectly computes the third derivative term, and choice D subtracts the linear approximation from the actual value.
  2. If P2(x)P_2(x) is the second-degree Taylor polynomial for f(x)=ln⁡(1+x)f(x) = \ln(1 + x) centered at x=0x = 0, and Q2(x)Q_2(x) is the second-degree Taylor polynomial for g(x)=ln⁡(1+2x)g(x) = \ln(1 + 2x) centered at x=0x = 0, which relationship between P2(x)P_2(x) and Q2(x)Q_2(x) is correct?
    Answer: Q2(x)=P2(2x)Q_2(x) = P_2(2x) for all values of xx For ln⁡(1+x)\ln(1+x): P2(x)=x−x22P_2(x) = x - \frac{x^2}{2}. For ln⁡(1+2x)\ln(1+2x): the derivatives at x=0x=0 are f′(0)=2f'(0) = 2, f′′(0)=−4f''(0) = -4, so Q2(x)=2x−4x22=2x−2x2Q_2(x) = 2x - \frac{4x^2}{2} = 2x - 2x^2. Note that P2(2x)=2x−(2x)22=2x−2x2=Q2(x)P_2(2x) = 2x - \frac{(2x)^2}{2} = 2x - 2x^2 = Q_2(x). Choice A gives 2P2(x)=2x−x2≠Q2(x)2P_2(x) = 2x - x^2 \neq Q_2(x). Choice C is the same as A. Choice D adds an incorrect correction term.
  3. Consider the function h(x)=excos⁡(x)h(x) = e^x \cos(x). If the second-degree Taylor polynomial for h(x)h(x) centered at x=0x = 0 is P2(x)=a0+a1x+a2x2P_2(x) = a_0 + a_1 x + a_2 x^2, what is the value of a2a_2?
    Answer: a2=0a_2 = 0 from the second derivative evaluation at x=0x = 0 Using the product rule: h′(x)=excos⁡(x)−exsin⁡(x)h'(x) = e^x \cos(x) - e^x \sin(x) and h′′(x)=excos⁡(x)−exsin⁡(x)−exsin⁡(x)−excos⁡(x)=−2exsin⁡(x)h''(x) = e^x \cos(x) - e^x \sin(x) - e^x \sin(x) - e^x \cos(x) = -2e^x \sin(x). At x=0x = 0: h(0)=1h(0) = 1, h′(0)=1h'(0) = 1, and h′′(0)=−2e0sin⁡(0)=0h''(0) = -2e^0 \sin(0) = 0. Therefore a2=h′′(0)2!=0a_2 = \frac{h''(0)}{2!} = 0. Choice A gives the right answer but wrong reasoning. Choice B incorrectly applies the product rule. Choice C assumes h′′(0)=−1h''(0) = -1 which is incorrect.
  4. The third-degree Taylor polynomial for f(x)=1+xf(x) = \sqrt{1 + x} centered at x=0x = 0 is used to approximate 1.08\sqrt{1.08}. Which calculation setup is correct for finding this approximation?
    Answer: P3(0.08)=1+12(0.08)−18(0.08)2+116(0.08)3P_3(0.08) = 1 + \frac{1}{2}(0.08) - \frac{1}{8}(0.08)^2 + \frac{1}{16}(0.08)^3 For f(x)=(1+x)1/2f(x) = (1+x)^{1/2}, we need: f(0)=1f(0) = 1, f′(x)=12(1+x)−1/2⇒f′(0)=12f'(x) = \frac{1}{2}(1+x)^{-1/2} \Rightarrow f'(0) = \frac{1}{2}, f′′(x)=−14(1+x)−3/2⇒f′′(0)=−14f''(x) = -\frac{1}{4}(1+x)^{-3/2} \Rightarrow f''(0) = -\frac{1}{4}, f′′′(x)=38(1+x)−5/2⇒f′′′(0)=38f'''(x) = \frac{3}{8}(1+x)^{-5/2} \Rightarrow f'''(0) = \frac{3}{8}. So P3(x)=1+12x+−1/42!x2+3/83!x3=1+12x−18x2+116x3P_3(x) = 1 + \frac{1}{2}x + \frac{-1/4}{2!}x^2 + \frac{3/8}{3!}x^3 = 1 + \frac{1}{2}x - \frac{1}{8}x^2 + \frac{1}{16}x^3. Choice B has wrong sign on the cubic term. Choice C uses wrong coefficients. Choice D has wrong signs on the quadratic and cubic terms.
  5. Two functions f(x)f(x) and g(x)g(x) have the same second-degree Taylor polynomial P2(x)=2+3x−x2P_2(x) = 2 + 3x - x^2 centered at x=0x = 0. If f(0.1)=2.29f(0.1) = 2.29 and the second-degree Taylor polynomial approximation gives P2(0.1)=2.29P_2(0.1) = 2.29, what can be concluded about f′′′(0)f'''(0)?
    Answer: f′′′(0)f'''(0) cannot be determined from the given information The fact that f(0.1)=P2(0.1)f(0.1) = P_2(0.1) is a coincidence at this particular point and doesn't imply anything about f′′′(0)f'''(0). The Taylor remainder theorem shows that f(0.1)−P2(0.1)=f′′′(c)3!(0.1)3f(0.1) - P_2(0.1) = \frac{f'''(c)}{3!}(0.1)^3 for some cc between 0 and 0.1. Since this equals zero, we know f′′′(c)=0f'''(c) = 0 for some cc, but this doesn't determine f′′′(0)f'''(0). Choice A incorrectly assumes the derivative at 0 equals the derivative at the intermediate point. Choice C assumes f′′′(0)≠0f'''(0) \neq 0 without justification. Choice D incorrectly concludes the function must be polynomial.
  6. If Pn(x)P_n(x) represents the nnth-degree Taylor polynomial for sin⁡(x)\sin(x) centered at x=0x = 0, which statement about P4(x)P_4(x) and P5(x)P_5(x) is correct?
    Answer: P5(x)=P4(x)+x55!P_5(x) = P_4(x) + \frac{x^5}{5!} with the additional term being positive The Taylor series for sin⁡(x)\sin(x) is x−x33!+x55!−x77!+⋯x - \frac{x^3}{3!} + \frac{x^5}{5!} - \frac{x^7}{7!} + \cdots. Since there is no x4x^4 term, P4(x)=x−x36P_4(x) = x - \frac{x^3}{6}. The x5x^5 term has coefficient +15!+\frac{1}{5!} (positive in the alternating series), so P5(x)=x−x36+x5120=P4(x)+x55!P_5(x) = x - \frac{x^3}{6} + \frac{x^5}{120} = P_4(x) + \frac{x^5}{5!}. Choice A incorrectly identifies which term is missing. Choice B is wrong about both the reasoning and which polynomial has the missing term. Choice D has the wrong sign for the x5x^5 coefficient.
  7. The function k(x)=ln⁡(cos⁡(x))k(x) = \ln(\cos(x)) is approximated by its second-degree Taylor polynomial centered at x=0x = 0. Which expression represents this polynomial?
    Answer: P2(x)=−x22P_2(x) = -\frac{x^2}{2} since ln⁡(1)=0\ln(1) = 0 and odd derivatives vanish We have k(0)=ln⁡(cos⁡(0))=ln⁡(1)=0k(0) = \ln(\cos(0)) = \ln(1) = 0. For the derivatives: k′(x)=−sin⁡(x)cos⁡(x)=−tan⁡(x)k'(x) = \frac{-\sin(x)}{\cos(x)} = -\tan(x), so k′(0)=0k'(0) = 0. k′′(x)=−sec⁡2(x)k''(x) = -\sec^2(x), so k′′(0)=−1k''(0) = -1. Therefore P2(x)=0+0⋅x+−12!x2=−x22P_2(x) = 0 + 0 \cdot x + \frac{-1}{2!}x^2 = -\frac{x^2}{2}. Choice B incorrectly starts with 1 instead of 0. Choice C uses wrong derivative calculations. Choice D includes a fourth-degree term which exceeds the requested degree, and the coefficient is incorrect anyway.

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