Taylor & Maclaurin Series - Calculus 2

  1. If h(x)=xcos⁡(x3)h(x) = x \cos(x^3), what is the coefficient of x7x^7 in the Maclaurin series for h(x)h(x)?
    Answer: −12-\frac{1}{2} When finding coefficients in Maclaurin series for products of functions, you need to systematically expand each factor and identify which terms contribute to your target power. Start with the Maclaurin series for cos⁡(u)=1−u22!+u44!−u66!+⋯\cos(u) = 1 - \frac{u^2}{2!} + \frac{u^4}{4!} - \frac{u^6}{6!} + \cdots. Substituting u=x3u = x^3: cos⁡(x3)=1−(x3)22!+(x3)44!−(x3)66!+⋯=1−x62+x1224−x18720+⋯\cos(x^3) = 1 - \frac{(x^3)^2}{2!} + \frac{(x^3)^4}{4!} - \frac{(x^3)^6}{6!} + \cdots = 1 - \frac{x^6}{2} + \frac{x^{12}}{24} - \frac{x^{18}}{720} + \cdots Now multiply by xx: h(x)=xcos⁡(x3)=x(1−x62+x1224−⋯ )=x−x72+x1324−⋯h(x) = x \cos(x^3) = x\left(1 - \frac{x^6}{2} + \frac{x^{12}}{24} - \cdots\right) = x - \frac{x^7}{2} + \frac{x^{13}}{24} - \cdots The coefficient of x7x^7 is −12-\frac{1}{2}, confirming answer D. Let's examine the wrong answers: A) −16-\frac{1}{6} likely comes from incorrectly using 13!\frac{1}{3!} instead of 12!\frac{1}{2!} when expanding cos⁡(x3)\cos(x^3). B) −1120-\frac{1}{120} suggests confusion with 15!\frac{1}{5!}, perhaps from misidentifying which factorial applies. C) 16\frac{1}{6} combines the factorial error from option A with a sign error—forgetting that the x6x^6 term in cos⁡(x3)\cos(x^3) comes from the negative −u22!-\frac{u^2}{2!} term. Study tip: When working with Maclaurin series of composite functions, write out the first several terms explicitly rather than trying to work with general formulas. This prevents factorial and sign errors that are common in these problems.
  2. Find the Taylor series representation for f(x)=1x2 f(x) = \frac{1}{x^2} centered at a=−1a = -1.
    Answer: ∑n=0∞(n+1)(x+1)n \sum_{n=0}^{\infty} (n+1) (x+1)^n We need to find the Taylor series for f(x)=x−2f(x) = x^{-2} centered at a=−1a = -1. We'll compute the derivatives and evaluate them at x=−1x = -1. f(x)=x−2  ⟹  f(−1)=1f(x) = x^{-2} \implies f(-1) = 1 f′(x)=−2x−3  ⟹  f′(−1)=2f'(x) = -2x^{-3} \implies f'(-1) = 2 f′′(x)=6x−4  ⟹  f′′(−1)=6f''(x) = 6x^{-4} \implies f''(-1) = 6 f′′′(x)=−24x−5  ⟹  f′′′(−1)=24f'''(x) = -24x^{-5} \implies f'''(-1) = 24 In general, f(n)(x)=(−1)n(n+1)!x−(n+2)f^{(n)}(x) = (-1)^n (n+1)! x^{-(n+2)}. Evaluating at x=−1x = -1: f(n)(−1)=(−1)n(n+1)!(−1)−(n+2)=(n+1)!f^{(n)}(-1) = (-1)^n (n+1)! (-1)^{-(n+2)} = (n+1)!. The Taylor series coefficient is cn=f(n)(−1)n!=(n+1)!n!=n+1c_n = \frac{f^{(n)}(-1)}{n!} = \frac{(n+1)!}{n!} = n+1. Therefore, the Taylor series is ∑n=0∞(n+1)(x+1)n\sum_{n=0}^{\infty} (n+1)(x+1)^n.
  3. What is the coefficient of x4x^4 in the Maclaurin series expansion for the function f(x)=sin⁡(x)1−xf(x) = \frac{\sin(x)}{1-x}?
    Answer: 56 \frac{5}{6} To find the coefficient, multiply the Maclaurin series for sin⁡(x)\sin(x) and 11−x\frac{1}{1-x}. sin⁡(x)=x−x33!+x55!−… \sin(x) = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \dots 11−x=1+x+x2+x3+x4+… \frac{1}{1-x} = 1 + x + x^2 + x^3 + x^4 + \dots Multiplying these two series, we look for the terms that produce x4x^4: (x)(x3)+(−x36)(x)=x4−16x4=(1−16)x4=56x4 (x)(x^3) + \left(-\frac{x^3}{6}\right)(x) = x^4 - \frac{1}{6}x^4 = \left(1 - \frac{1}{6}\right)x^4 = \frac{5}{6}x^4 The coefficient is 56\frac{5}{6}.
  4. The function f(x)=12−xf(x) = \frac{1}{2-x} can be written as a Maclaurin series. What is the radius of convergence of this series?
    Answer: R=2R = 2 When you encounter a rational function like f(x)=12−xf(x) = \frac{1}{2-x} and need to find the radius of convergence of its Maclaurin series, look for where the function has singularities (points where it's undefined or discontinuous). To find the Maclaurin series, you can rewrite this function in a form that matches a known series. Factor out the constant: f(x)=12−x=12⋅11−x2f(x) = \frac{1}{2-x} = \frac{1}{2} \cdot \frac{1}{1-\frac{x}{2}}. This matches the geometric series formula 11−u=∑n=0∞un\frac{1}{1-u} = \sum_{n=0}^{\infty} u^n where u=x2u = \frac{x}{2}, which converges when ∣u∣<1|u| < 1. For convergence, you need ∣x2∣<1\left|\frac{x}{2}\right| < 1, which means ∣x∣<2|x| < 2. Therefore, the radius of convergence is R=2R = 2, making (D) correct. The wrong answers represent common misconceptions: (A) R=1R = 1 might come from forgetting the factor of 2 in the denominator and treating this like 11−x\frac{1}{1-x}. (C) R=12R = \frac{1}{2} could result from incorrectly thinking the radius equals the coefficient 12\frac{1}{2} or making an algebraic error. (B) R=∞R = \infty would suggest the series converges everywhere, but rational functions with finite poles never have infinite radius of convergence. Study tip: For rational functions, the radius of convergence equals the distance from the center of expansion (here, x=0x = 0) to the nearest singularity. Since f(x)f(x) has a pole at x=2x = 2, the radius is ∣2−0∣=2|2 - 0| = 2.
  5. If the Maclaurin series for f(x)f(x) is ∑n=1∞(−1)n+1xnn2 \sum_{n=1}^{\infty} \frac{(-1)^{n+1} x^n}{n^2} , what is the Maclaurin series for f′(x)f'(x)?
    Answer: ∑k=0∞(−1)kxkk+1 \sum_{k=0}^{\infty} \frac{(-1)^k x^k}{k+1} We differentiate the series for f(x)f(x) term-by-term to find the series for f′(x)f'(x). f′(x)=ddx(∑n=1∞(−1)n+1xnn2)=∑n=1∞(−1)n+1(nxn−1)n2=∑n=1∞(−1)n+1xn−1n f'(x) = \frac{d}{dx} \left( \sum_{n=1}^{\infty} \frac{(-1)^{n+1} x^n}{n^2} \right) = \sum_{n=1}^{\infty} \frac{(-1)^{n+1} (n x^{n-1})}{n^2} = \sum_{n=1}^{\infty} \frac{(-1)^{n+1} x^{n-1}}{n} To match the format of the answer choices, we re-index the series. Let k=n−1k = n-1, so n=k+1n = k+1. When n=1n=1, k=0k=0. The sum becomes: ∑k=0∞(−1)(k+1)+1xkk+1=∑k=0∞(−1)k+2xkk+1=∑k=0∞(−1)kxkk+1 \sum_{k=0}^{\infty} \frac{(-1)^{(k+1)+1} x^k}{k+1} = \sum_{k=0}^{\infty} \frac{(-1)^{k+2} x^k}{k+1} = \sum_{k=0}^{\infty} \frac{(-1)^k x^k}{k+1} This is the Maclaurin series for ln⁡(1+x)x\frac{\ln(1+x)}{x}.
  6. What is the Maclaurin series for f(x)=cosh⁡(x)=ex+e−x2f(x) = \cosh(x) = \frac{e^x + e^{-x}}{2}?
    Answer: ∑n=0∞x2n(2n)! \sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!} We use the Maclaurin series for exe^x and e−xe^{-x}. ex=1+x+x22!+x33!+x44!+…e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \dots e−x=1−x+x22!−x33!+x44!−…e^{-x} = 1 - x + \frac{x^2}{2!} - \frac{x^3}{3!} + \frac{x^4}{4!} - \dots Adding them together, the odd-powered terms cancel: ex+e−x=2+2x22!+2x44!+⋯=2∑n=0∞x2n(2n)!e^x + e^{-x} = 2 + 2\frac{x^2}{2!} + 2\frac{x^4}{4!} + \dots = 2 \sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!} Dividing by 2 gives the series for cosh⁡(x)\cosh(x): ∑n=0∞x2n(2n)!\sum_{n=0}^{\infty} \frac{x^{2n}}{(2n)!}.
  7. Which of the following is the Taylor series for f(x)=sin⁡(x)f(x) = \sin(x) centered at a=π/2a = \pi/2?
    Answer: ∑n=0∞(−1)n(x−π/2)2n(2n)! \sum_{n=0}^{\infty} \frac{(-1)^n (x-\pi/2)^{2n}}{(2n)!} One way is to use a substitution and a trigonometric identity. Let u=x−π/2u = x - \pi/2, so x=u+π/2x = u + \pi/2. Then f(x)=sin⁡(u+π/2)f(x) = \sin(u + \pi/2). Using the angle addition formula, sin⁡(u+π/2)=sin⁡(u)cos⁡(π/2)+cos⁡(u)sin⁡(π/2)=cos⁡(u)\sin(u + \pi/2) = \sin(u)\cos(\pi/2) + \cos(u)\sin(\pi/2) = \cos(u). The Maclaurin series for cos⁡(u)\cos(u) is ∑n=0∞(−1)nu2n(2n)!\sum_{n=0}^{\infty} \frac{(-1)^n u^{2n}}{(2n)!}. Substituting u=x−π/2u = x - \pi/2 back gives the Taylor series for sin⁡(x)\sin(x) at a=π/2a=\pi/2: ∑n=0∞(−1)n(x−π/2)2n(2n)!\sum_{n=0}^{\infty} \frac{(-1)^n (x-\pi/2)^{2n}}{(2n)!}.
  8. Find the Maclaurin series for the function f(x)=∫0xsin⁡(t)tdtf(x) = \int_0^x \frac{\sin(t)}{t} dt.
    Answer: ∑n=0∞(−1)nx2n+1(2n+1)!(2n+1) \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{(2n+1)!(2n+1)} First, find the Maclaurin series for sin⁡(t)\sin(t): sin⁡(t)=∑n=0∞(−1)nt2n+1(2n+1)!\sin(t) = \sum_{n=0}^{\infty} \frac{(-1)^n t^{2n+1}}{(2n+1)!}. Next, divide by tt: sin⁡(t)t=∑n=0∞(−1)nt2n(2n+1)!\frac{\sin(t)}{t} = \sum_{n=0}^{\infty} \frac{(-1)^n t^{2n}}{(2n+1)!}. Finally, integrate term-by-term from 0 to xx: ∫0x∑n=0∞(−1)nt2n(2n+1)!dt=∑n=0∞(−1)n(2n+1)!∫0xt2ndt=∑n=0∞(−1)n(2n+1)![t2n+12n+1]0x=∑n=0∞(−1)nx2n+1(2n+1)!(2n+1) \int_0^x \sum_{n=0}^{\infty} \frac{(-1)^n t^{2n}}{(2n+1)!} dt = \sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} \int_0^x t^{2n} dt = \sum_{n=0}^{\infty} \frac{(-1)^n}{(2n+1)!} \left[ \frac{t^{2n+1}}{2n+1} \right]_0^x = \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{(2n+1)!(2n+1)}
  9. Find the Taylor series for f(x)=e3xf(x) = e^{3x} centered at a=−1a=-1.
    Answer: ∑n=0∞3ne−3(x+1)nn! \sum_{n=0}^{\infty} \frac{3^n e^{-3} (x+1)^n}{n!} When finding a Taylor series centered at a point other than zero, you need to use the general Taylor series formula and carefully evaluate all derivatives at the given center point. For f(x)=e3xf(x) = e^{3x} centered at a=−1a = -1, start by finding the pattern of derivatives. The first few derivatives are: f′(x)=3e3xf'(x) = 3e^{3x}, f′′(x)=9e3xf''(x) = 9e^{3x}, f′′′(x)=27e3xf'''(x) = 27e^{3x}. In general, f(n)(x)=3ne3xf^{(n)}(x) = 3^n e^{3x}. Next, evaluate each derivative at the center point x=−1x = -1: f(n)(−1)=3ne3(−1)=3ne−3f^{(n)}(-1) = 3^n e^{3(-1)} = 3^n e^{-3}. The Taylor series formula gives us: f(x)=∑n=0∞f(n)(−1)n!(x−(−1))n=∑n=0∞3ne−3n!(x+1)nf(x) = \sum_{n=0}^{\infty} \frac{f^{(n)}(-1)}{n!}(x-(-1))^n = \sum_{n=0}^{\infty} \frac{3^n e^{-3}}{n!}(x+1)^n This matches choice C exactly. Looking at the wrong answers: Choice A is missing the 3n3^n factor that comes from the chain rule when differentiating e3xe^{3x}. Choice B incorrectly uses e3e^3 instead of e−3e^{-3} - this happens when you forget to substitute x=−1x = -1 and mistakenly use x=1x = 1. Choice D has the wrong center point, using (x−1)(x-1) instead of (x+1)(x+1), and is missing the exponential factor entirely. Study tip: Always substitute the center point into your derivatives carefully, and remember that centering at a=−1a = -1 means your series involves (x+1)(x+1) terms, not (x−1)(x-1).
  10. The Maclaurin series for f(x)=(1−x)−2f(x) = (1-x)^{-2} is ∑n=0∞(n+1)xn\sum_{n=0}^{\infty} (n+1)x^n. What is f(10)(0)f^{(10)}(0)?
    Answer: 11! 11! The coefficient of xnx^n in the Maclaurin series is cn=f(n)(0)n!c_n = \frac{f^{(n)}(0)}{n!}. From the given series, the coefficient of xnx^n is cn=n+1c_n = n+1. We want to find f(10)(0)f^{(10)}(0), so we look at the case where n=10n=10. The coefficient is c10=10+1=11c_{10} = 10+1 = 11. Using the formula, c10=f(10)(0)10!c_{10} = \frac{f^{(10)}(0)}{10!}. So, 11=f(10)(0)10!11 = \frac{f^{(10)}(0)}{10!}. Solving for the derivative gives f(10)(0)=11⋅10!=11!f^{(10)}(0) = 11 \cdot 10! = 11!.
  11. Use the provided information to find the Maclaurin series for g(x)=11+x2g(x) = \frac{1}{1+x^2}.
    Answer: ∑n=0∞(−1)nx2n \sum_{n=0}^{\infty} (-1)^n x^{2n} We know that the derivative of arctan⁡(x)\arctan(x) is 11+x2\frac{1}{1+x^2}. Therefore, we can find the series for g(x)g(x) by differentiating the series for arctan⁡(x)\arctan(x) term-by-term. g(x)=ddx(∑n=0∞(−1)nx2n+12n+1)=∑n=0∞ddx((−1)nx2n+12n+1) g(x) = \frac{d}{dx} \left( \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{2n+1} \right) = \sum_{n=0}^{\infty} \frac{d}{dx} \left( \frac{(-1)^n x^{2n+1}}{2n+1} \right) =∑n=0∞(−1)n(2n+1)x2n2n+1=∑n=0∞(−1)nx2n = \sum_{n=0}^{\infty} \frac{(-1)^n (2n+1)x^{2n}}{2n+1} = \sum_{n=0}^{\infty} (-1)^n x^{2n} This is also recognizable as the geometric series for 11−(−x2)\frac{1}{1-(-x^2)}.
  12. Find the first four terms of the Taylor series for f(x)=12−xf(x) = \frac{1}{2-x} centered at a=1a=1.
    Answer: 1+(x−1)+(x−1)2+(x−1)3 1 + (x-1) + (x-1)^2 + (x-1)^3 The most efficient method is to manipulate the function into the form of a geometric series, 11−r\frac{1}{1-r}. f(x)=12−x=12−(1+(x−1))=11−(x−1) f(x) = \frac{1}{2-x} = \frac{1}{2 - (1 + (x-1))} = \frac{1}{1 - (x-1)} This is a geometric series with first term a=1a=1 and common ratio r=x−1r = x-1. The series is ∑n=0∞(x−1)n\sum_{n=0}^{\infty} (x-1)^n. The first four terms (for n=0,1,2,3n=0, 1, 2, 3) are 1+(x−1)+(x−1)2+(x−1)31 + (x-1) + (x-1)^2 + (x-1)^3.
  13. Find the first three non-zero terms of the Taylor series for g(x)=ln⁡(1+x2)g(x) = \ln(1 + x^2) centered at x=0x = 0.
    Answer: x2−x42+x63x^2 - \frac{x^4}{2} + \frac{x^6}{3} Using the known series ln⁡(1+u)=u−u22+u33−u44+⋯\ln(1 + u) = u - \frac{u^2}{2} + \frac{u^3}{3} - \frac{u^4}{4} + \cdots and substituting u=x2u = x^2: ln⁡(1+x2)=x2−(x2)22+(x2)33−⋯=x2−x42+x63−⋯\ln(1 + x^2) = x^2 - \frac{(x^2)^2}{2} + \frac{(x^2)^3}{3} - \cdots = x^2 - \frac{x^4}{2} + \frac{x^6}{3} - \cdots. Choice B incorrectly has x8x^8 instead of x6x^6 in the third term. Choice C includes the constant term 1, which doesn't appear since ln⁡(1)=0\ln(1) = 0. Choice D uses the original ln⁡(1+u)\ln(1+u) series without substituting u=x2u = x^2.
  14. Consider the function f(x)=cos⁡(x)sin⁡(x)f(x) = \cos(x) \sin(x). The Maclaurin series for f(x)f(x) has the form ∑n=0∞anxn\sum_{n=0}^{\infty} a_n x^n. Which of the following statements about the coefficients is true?
    Answer: a1=1a_1 = 1 and a3=−23a_3 = -\frac{2}{3}, with all even coefficients zero Using the identity cos⁡(x)sin⁡(x)=12sin⁡(2x)\cos(x)\sin(x) = \frac{1}{2}\sin(2x), we can find the Maclaurin series: f(x)=12sin⁡(2x)=12[2x−(2x)33!+(2x)55!−⋯ ]=x−8x312+⋯=x−2x33+⋯f(x) = \frac{1}{2}\sin(2x) = \frac{1}{2}[2x - \frac{(2x)^3}{3!} + \frac{(2x)^5}{5!} - \cdots] = x - \frac{8x^3}{12} + \cdots = x - \frac{2x^3}{3} + \cdots. So a1=1a_1 = 1 and a3=−23a_3 = -\frac{2}{3}. Since sin⁡(2x)\sin(2x) only has odd powers, all even coefficients are zero. Choice A incorrectly gives a non-zero even coefficient. Choice B incorrectly claims odd coefficients are zero for k≥1k \geq 1. Choice D incorrectly has a2=1a_2 = 1.
  15. Let f(x)f(x) be a function such that f(1)=2f(1) = 2, f′(1)=−1f'(1) = -1, f′′(1)=6f''(1) = 6, and f′′′(1)=−12f'''(1) = -12. What is the third-degree Taylor polynomial, T3(x)T_3(x), for f(x)f(x) centered at a=1a = 1?
    Answer: 2−(x−1)+3(x−1)2−2(x−1)3 2 - (x-1) + 3(x-1)^2 - 2(x-1)^3 The formula for the third-degree Taylor polynomial centered at a=1a=1 is: T3(x)=f(1)+f′(1)1!(x−1)+f′′(1)2!(x−1)2+f′′′(1)3!(x−1)3 T_3(x) = f(1) + \frac{f'(1)}{1!}(x-1) + \frac{f''(1)}{2!}(x-1)^2 + \frac{f'''(1)}{3!}(x-1)^3 Substituting the given values: T3(x)=2+−11(x−1)+62(x−1)2+−126(x−1)3 T_3(x) = 2 + \frac{-1}{1}(x-1) + \frac{6}{2}(x-1)^2 + \frac{-12}{6}(x-1)^3 T3(x)=2−(x−1)+3(x−1)2−2(x−1)3 T_3(x) = 2 - (x-1) + 3(x-1)^2 - 2(x-1)^3 Distractor (A) forgets to divide by the factorials. Distractor (C) incorrectly centers the polynomial at 0. Distractor (D) makes an error in calculating 3!3!.
  16. Which function is represented by the Maclaurin series ∑n=0∞(−1)n(2x)2n+1(2n+1)! \sum_{n=0}^{\infty} \frac{(-1)^n (2x)^{2n+1}}{(2n+1)!} ?
    Answer: sin⁡(2x) \sin(2x) The standard Maclaurin series for sin⁡(u)\sin(u) is ∑n=0∞(−1)nu2n+1(2n+1)!\sum_{n=0}^{\infty} \frac{(-1)^n u^{2n+1}}{(2n+1)!}. The given series has the same form, ∑n=0∞(−1)n(2x)2n+1(2n+1)! \sum_{n=0}^{\infty} \frac{(-1)^n (2x)^{2n+1}}{(2n+1)!} . By comparing the two series, we can see that u=2xu = 2x. Therefore, the function represented by the series is sin⁡(2x)\sin(2x).
  17. What is the Maclaurin series for the function f(x)=xarctan⁡(x2)f(x) = x \arctan(x^2)?
    Answer: ∑n=0∞(−1)nx4n+32n+1 \sum_{n=0}^{\infty} \frac{(-1)^n x^{4n+3}}{2n+1} When you encounter a Maclaurin series problem involving composite functions like xarctan⁡(x2)x \arctan(x^2), start with known series and use substitution rather than computing derivatives from scratch. The key insight is to recall the Maclaurin series for arctan⁡(u)\arctan(u): arctan⁡(u)=∑n=0∞(−1)nu2n+12n+1\arctan(u) = \sum_{n=0}^{\infty} \frac{(-1)^n u^{2n+1}}{2n+1}. This series is valid for ∣u∣≤1|u| \leq 1. To find the series for arctan⁡(x2)\arctan(x^2), substitute u=x2u = x^2: arctan⁡(x2)=∑n=0∞(−1)n(x2)2n+12n+1=∑n=0∞(−1)nx4n+22n+1\arctan(x^2) = \sum_{n=0}^{\infty} \frac{(-1)^n (x^2)^{2n+1}}{2n+1} = \sum_{n=0}^{\infty} \frac{(-1)^n x^{4n+2}}{2n+1} Now multiply by xx to get f(x)=xarctan⁡(x2)f(x) = x \arctan(x^2): xarctan⁡(x2)=x⋅∑n=0∞(−1)nx4n+22n+1=∑n=0∞(−1)nx4n+32n+1x \arctan(x^2) = x \cdot \sum_{n=0}^{\infty} \frac{(-1)^n x^{4n+2}}{2n+1} = \sum_{n=0}^{\infty} \frac{(-1)^n x^{4n+3}}{2n+1} This confirms answer C. Looking at the wrong answers: A gives you arctan⁡(x2)\arctan(x^2) but forgets the multiplication by xx. B has the wrong exponent pattern—it would come from xarctan⁡(x)x \arctan(x) instead of xarctan⁡(x2)x \arctan(x^2). D is missing the alternating signs (−1)n(-1)^n, which are essential in the arctangent series. Study tip: For composite function series, always start with a known series and substitute carefully. Keep track of every transformation—substitution, then multiplication—and verify your exponent patterns match the operations you performed.
  18. Let Tn(x)T_n(x) denote the nn-th degree Taylor polynomial of f(x)=ln⁡(1+x)f(x) = \ln(1+x) at x=0x=0. Which of the following is T3(x)T_3(x)?
    Answer: x−x22+x33 x - \frac{x^2}{2} + \frac{x^3}{3} The Maclaurin series for ln⁡(1+x)\ln(1+x) is a standard series: ln⁡(1+x)=∑n=1∞(−1)n−1xnn=x−x22+x33−x44+… \ln(1+x) = \sum_{n=1}^{\infty} \frac{(-1)^{n-1}x^n}{n} = x - \frac{x^2}{2} + \frac{x^3}{3} - \frac{x^4}{4} + \dots The third-degree Taylor polynomial, T3(x)T_3(x), consists of all terms up to and including the degree 3 term. Thus, T3(x)=x−x22+x33T_3(x) = x - \frac{x^2}{2} + \frac{x^3}{3}.
  19. The Maclaurin series for a function f(x)f(x) is given by ∑n=0∞(n+1)2nxn \sum_{n=0}^{\infty} (n+1)2^n x^n . What is the value of f′′′(0)f'''(0)?
    Answer: 192 192 The coefficient of xnx^n in a Maclaurin series is given by cn=f(n)(0)n!c_n = \frac{f^{(n)}(0)}{n!}. We want f′′′(0)f'''(0), so we need the coefficient of the n=3n=3 term, c3c_3. From the given series, cn=(n+1)2nc_n = (n+1)2^n. For n=3n=3, c3=(3+1)23=4⋅8=32c_3 = (3+1)2^3 = 4 \cdot 8 = 32. Now, we solve for the derivative: f′′′(0)=c3⋅3!=32⋅6=192f'''(0) = c_3 \cdot 3! = 32 \cdot 6 = 192.
  20. Which of the following is the Taylor series for f(x)=ln⁡(x)f(x) = \ln(x) centered at a=2a = 2?
    Answer: ln⁡(2)+∑n=1∞(−1)n−1(x−2)nn⋅2n \ln(2) + \sum_{n=1}^{\infty} \frac{(-1)^{n-1}(x-2)^n}{n \cdot 2^n} To find the Taylor series, we compute the derivatives of f(x)=ln⁡(x)f(x) = \ln(x) at a=2a=2. f(2)=ln⁡(2)f(2) = \ln(2). f′(x)=x−1f'(x) = x^{-1}, f′′(x)=−x−2f''(x) = -x^{-2}, f′′′(x)=2x−3f'''(x) = 2x^{-3}, and in general, f(n)(x)=(−1)n−1(n−1)!x−nf^{(n)}(x) = (-1)^{n-1}(n-1)!x^{-n} for n≥1n \ge 1. At a=2a=2, f(n)(2)=(−1)n−1(n−1)!2nf^{(n)}(2) = \frac{(-1)^{n-1}(n-1)!}{2^n}. The Taylor series coefficient is cn=f(n)(2)n!=(−1)n−1(n−1)!n!⋅2n=(−1)n−1n⋅2nc_n = \frac{f^{(n)}(2)}{n!} = \frac{(-1)^{n-1}(n-1)!}{n! \cdot 2^n} = \frac{(-1)^{n-1}}{n \cdot 2^n} for n≥1n \ge 1. The series is f(2)+∑n=1∞cn(x−2)nf(2) + \sum_{n=1}^{\infty} c_n (x-2)^n, which is ln⁡(2)+∑n=1∞(−1)n−1(x−2)nn⋅2n\ln(2) + \sum_{n=1}^{\infty} \frac{(-1)^{n-1}(x-2)^n}{n \cdot 2^n}.

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