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Chapter 6 Solutions

Worked solutions to all thirty problems, with the reason for each step. These explanations were added for this edition; the chapter answer key and original worked examples follow below.

Chapter problems →

Problem 1

Original problem · added worked solution

What is the definition of a power series?

  1. Choose a center c and a fixed sequence of coefficients a0,a1,…a_0,a_1,….
  2. A power series has the form ∑n=0∞an(x-c)n∑_{n=0}^{∞}a_n(x-c)^n. Each term is a constant coefficient times a nonnegative integer power of the distance from the center.
  3. Convergence is assessed at each x; the center always converges to a0a_0.

Final answer

A series ∑n=0∞an(x-c)n∑_{n=0}^{∞}a_n(x-c)^n with constant coefficients and center c.

Problem 2

Original problem · added worked solution

What is the definition of a power series?

  1. Choose a center c and a fixed sequence of coefficients a0,a1,…a_0,a_1,….
  2. A power series has the form ∑n=0∞an(x-c)n∑_{n=0}^{∞}a_n(x-c)^n. Each term is a constant coefficient times a nonnegative integer power of the distance from the center.
  3. Convergence is assessed at each x; the center always converges to a0a_0.

Final answer

A series ∑n=0∞an(x-c)n∑_{n=0}^{∞}a_n(x-c)^n with constant coefficients and center c.

Problem 3

Original problem · clarified · added worked solution

Prove that f(x)g(x)=∑n=0∞(∑i=0naibn-i)(x-c)nf(x)g(x)=∑_{n=0}^{∞}(∑_{i=0}^{n}a_i b_{n-i})(x-c)^n.

Clarified version: the inner sum ends at n, so it includes exactly the coefficient pairs whose indices add to n.

  1. Write f(x)=∑i=0∞ai(x-c)if(x)=∑_{i=0}^{∞}a_i(x-c)^i and g(x)=∑j=0∞bj(x-c)jg(x)=∑_{j=0}^{∞}b_j(x-c)^j. Work where both series converge absolutely, in particular inside their common radius.
  2. Set t=x-ct=x-c. The product of the i-th and j-th terms is aibjti+ja_i b_j t^{i+j}. A term has total degree n exactly when i+j=ni+j=n.
  3. For a fixed n, the possible indices are i=0,1,…,ni=0,1,…,n, with j=n-ij=n-i. Therefore the coefficient of tⁿ is ∑i=0naibn-i∑_{i=0}^{n}a_i b_{n-i}.
  4. The absolute double sum is ∑i=0∞∑j=0∞|aibjti+j|=(∑i=0∞|aiti|)(∑j=0∞|bjtj|)<∞∑_{i=0}^{∞}∑_{j=0}^{∞}|a_i b_j t^{i+j}|=(∑_{i=0}^{∞}|a_i t^i|)(∑_{j=0}^{∞}|b_j t^j|)<∞. Absolute convergence permits grouping terms by total degree. This proves the stated product identity.

Final answer

f(x)g(x)=∑n=0∞(∑i=0naibn-i)(x-c)nf(x)g(x)=∑_{n=0}^{∞}(∑_{i=0}^{n}a_i b_{n-i})(x-c)^n, wherever both power series converge absolutely.

Problem 4

Original problem · clarified · added worked solution

For f(x)=∑n=0∞n2xnf(x)=∑_{n=0}^{∞}n^2x^n and g(x)=∑n=0∞(2n+1)xng(x)=∑_{n=0}^{∞}(2n+1)x^n compute the following.

  1. f(x)+g(x)f(x)+g(x)
  2. f(x)-g(x)f(x)-g(x)
  3. df/dxdf/dx
  4. ∫g(x)dx∫g(x)dx

Clarified version: g(x) includes the factor xⁿ in each term, making it a power series in x.

Both power series converge for |x|<1|x|<1 and diverge at x=±1 because their terms do not tend to zero. Perform the following operations inside |x|<1|x|<1.

(a)

  1. Add coefficients of matching powers: f(x)+g(x)=∑n=0∞(n2+2n+1)xn=∑n=0∞(n+1)2xnf(x)+g(x)=∑_{n=0}^{∞}(n^2+2n+1)x^n=∑_{n=0}^{∞}(n+1)^2x^n.
  2. Differentiate the geometric series to obtain ∑n=0∞nxn=x/(1-x)2∑_{n=0}^{∞}nx^n=x/(1-x)^2 and f(x)=x(1+x)/(1-x)3f(x)=x(1+x)/(1-x)^3. Also g(x)=2x/(1-x)2+1/(1-x)=(1+x)/(1-x)2g(x)=2x/(1-x)^2+1/(1-x)=(1+x)/(1-x)^2.
  3. Combining these rational functions gives f(x)+g(x)=(1+x)/(1-x)3f(x)+g(x)=(1+x)/(1-x)^3.

(b)

  1. Subtract coefficients of matching powers: f(x)-g(x)=∑n=0∞(n2-2n-1)xnf(x)-g(x)=∑_{n=0}^{∞}(n^2-2n-1)x^n.
  2. Using the rational forms from part (a), the common-denominator numerator is x(1+x)-(1+x)(1-x)=2x2+x-1x(1+x)-(1+x)(1-x)=2x^2+x-1.
  3. Thus f(x)-g(x)=(2x2+x-1)/(1-x)3f(x)-g(x)=(2x^2+x-1)/(1-x)^3.

(c)

  1. A power series can be differentiated term by term inside its radius. The n=0 term is zero, so f′(x)=∑n=1∞n3xn-1f′(x)=∑_{n=1}^{∞}n^3x^{n-1}.
  2. Differentiating x(1+x)/(1-x)3x(1+x)/(1-x)^3 by the product and chain rules gives f′(x)=(1+4x+x2)/(1-x)4f′(x)=(1+4x+x^2)/(1-x)^4.

(d)

  1. Integrate each term and include an arbitrary constant: ∫g(x)dx=C+∑n=0∞(2n+1)xn+1/(n+1)∫g(x)dx=C+∑_{n=0}^{∞}(2n+1)x^{n+1}/(n+1).
  2. Rewrite g(x)=2/(1-x)2-1/(1-x)g(x)=2/(1-x)^2-1/(1-x). Choose 2x/(1-x)2x/(1-x) as an antiderivative of the first term; its derivative is 2/(1-x)22/(1-x)^2. The second term integrates to ln(1-x)ln(1-x). Both chosen antiderivatives are zero at x=0, matching the integrated power series.
  3. Therefore an antiderivative is 2x/(1-x)+ln(1-x)+C2x/(1-x)+ln(1-x)+C. On |x|<1|x|<1, 1-x>01-x>0, so the logarithm is real.

Final answer

For |x|<1|x|<1: (a) (1+x)/(1-x)3(1+x)/(1-x)^3; (b) (2x2+x-1)/(1-x)3(2x^2+x-1)/(1-x)^3; (c) ∑n=1∞n3xn-1=(1+4x+x2)/(1-x)4∑_{n=1}^{∞}n^3x^{n-1}=(1+4x+x^2)/(1-x)^4; (d) C+∑n=0∞(2n+1)xn+1/(n+1)=2x/(1-x)+ln(1-x)+CC+∑_{n=0}^{∞}(2n+1)x^{n+1}/(n+1)=2x/(1-x)+ln(1-x)+C.

Problem 5

Original problem · added worked solution

Taylor expand the following function around the given value and note which are Maclaurin Series.

  1. Original source equation or figure
  2. Original source equation or figure
  3. Original source equation or figure
  4. Original source equation or figure
  5. Original source equation or figure
  6. Original source equation or figure
  7. Original source equation or figure

(a)

  1. Set h=x-3h=x-3, so the polynomial is (3+h)5-(3+h)3+1(3+h)^5-(3+h)^3+1.
  2. Use the binomial theorem and collect like powers. The result is 217+378h+261h2+89h3+15h4+h5217+378h+261h^2+89h^3+15h^4+h^5. This finite Taylor series is valid for every real x. The center is 3, so it is not Maclaurin.

(b)

  1. Set h=x-1h=x-1. Then (x-1)2/x=h2/(1+h)(x-1)^2/x=h^2/(1+h).
  2. Expand 1/(1+h)=∑n=0∞(-1)nhn1/(1+h)=∑_{n=0}^{∞}(-1)^n h^n for |h|<1|h|<1. Thus the answer is ∑n=0∞(-1)n(x-1)n+2∑_{n=0}^{∞}(-1)^n(x-1)^{n+2}. The terms do not vanish at either h endpoint. Its center is 1, so it is not Maclaurin.

(c)

  1. Integrate 1/(1-x)=∑n=0∞xn1/(1-x)=∑_{n=0}^{∞}x^n from zero to x and change the sign.
  2. This gives ln(1-x)=-∑n=1∞xn/nln(1-x)=-∑_{n=1}^{∞}x^n/n. It converges for -1≤x<1-1≤x<1: at −1 the alternating harmonic series converges, while at 1 the harmonic series diverges. Its center is 0, so it is Maclaurin.

(d)

  1. Set h=x-1h=x-1 and use cos(1+h)=cos(1)cos(h)-sin(1)sin(h)cos(1+h)=cos(1)cos(h)-sin(1)sin(h).
  2. Substitute the ordinary cosine and sine series: cos(1)∑n=0∞(-1)nh2n/(2n)!-sin(1)∑n=0∞(-1)nh2n+1/(2n+1)!cos(1)∑_{n=0}^{∞}(-1)^n h^{2n}/(2n)!-sin(1)∑_{n=0}^{∞}(-1)^n h^{2n+1}/(2n+1)!. It converges for all real h. The center is 1, so it is not Maclaurin.

(e)

  1. Set h=x-5h=x-5. Since ex=e5ehe^x=e^5e^h, substitute the exponential series.
  2. The result is e5∑n=0∞(x-5)n/n!e^5∑_{n=0}^{∞}(x-5)^n/n!, valid for all real x. The center is 5, so it is not Maclaurin.

(f)

  1. Expand 1/(1+x2)=∑n=0∞(-1)nx2n1/(1+x^2)=∑_{n=0}^{∞}(-1)^n x^{2n} inside |x|<1|x|<1 and integrate from 0 to x.
  2. This gives arctanx=∑n=0∞(-1)nx2n+1/(2n+1)arctan x=∑_{n=0}^{∞}(-1)^n x^{2n+1}/(2n+1). Both endpoints converge by the alternating series test, so the interval is -1≤x≤1-1≤x≤1. The center is 0, so it is Maclaurin.

(g)

  1. Start with ex=∑n=0∞xn/n!e^x=∑_{n=0}^{∞}x^n/n! and multiply each term by x.
  2. The result is xex=∑n=0∞xn+1/n!xe^x=∑_{n=0}^{∞}x^{n+1}/n!, valid for every real x. Its center is 0, so it is Maclaurin.

Final answer

The expansions are shown by part. Parts (c), (f), and (g) are Maclaurin series.

Problem 6

Added problem and worked solution

Find the radius and interval of convergence of ∑n=0∞xn∑_{n=0}^{∞}x^n.

  1. For an=xna_n=x^n, the geometric ratio is x, so convergence requires |x|<1|x|<1.
  2. At x=1 the terms are 1; at x=−1 they alternate ±1. Neither endpoint has terms tending to zero.

Final answer

Radius 1, interval (-1,1)(-1,1).

Problem 7

Added problem and worked solution

Find the center, radius, and interval of convergence of ∑n=0∞(x-2)n/3n∑_{n=0}^{∞}(x-2)^n/3^n.

  1. The series is geometric with ratio (x-2)/3(x-2)/3.
  2. Convergence requires |x-2|<3|x-2|<3, or -1<x<5-1<x<5. At each endpoint the ratio is ±1, so the terms fail the zero-limit test.

Final answer

Center 2, radius 3, interval (-1,5)(-1,5).

Problem 8

Added problem and worked solution

Find the radius and interval of convergence of ∑n=1∞xn/n∑_{n=1}^{∞}x^n/n.

  1. The ratio test gives a limit of |x||x|, so the radius is 1.
  2. At x=1, the harmonic series diverges. At x=−1, the alternating harmonic series converges. Outside radius 1 the terms do not approach zero.

Final answer

Radius 1, interval -1≤x<1-1≤x<1.

Problem 9

Added problem and worked solution

Find the radius and interval of convergence of ∑n=1∞xn/n2∑_{n=1}^{∞}x^n/n^2.

  1. The ratio of consecutive magnitudes tends to |x||x|, giving radius 1.
  2. At both endpoints the magnitudes are 1/n21/n^2, whose p-series converges. Both endpoints are included.

Final answer

Radius 1, interval -1≤x≤1-1≤x≤1.

Problem 10

Added problem and worked solution

Find the radius of convergence of ∑n=0∞xn/n!∑_{n=0}^{∞}x^n/n!.

  1. The ratio of consecutive magnitudes is |x|/(n+1)|x|/(n+1).
  2. This tends to zero for every fixed x. The ratio test therefore gives convergence for every real x.

Final answer

Infinite radius; all real x.

Problem 11

Added problem and worked solution

For which real x does ∑n=0∞n!xn∑_{n=0}^{∞}n!x^n converge?

  1. For nonzero x, the ratio of consecutive term magnitudes is (n+1)|x|(n+1)|x|, which tends to infinity. The terms eventually grow and the series diverges.
  2. At x=0, all positive-degree terms vanish and the constant term is 1.

Final answer

Radius 0; convergence only at x=0.

Problem 12

Added problem and worked solution

Differentiate the geometric power series to represent 1/(1-x)21/(1-x)^2. State the interval of convergence.

  1. The geometric series 1/(1-x)=∑n=0∞xn1/(1-x)=∑_{n=0}^{∞}x^n holds for |x|<1|x|<1.
  2. Differentiate term by term within the radius to obtain 1/(1-x)2=∑n=1∞nxn-11/(1-x)^2=∑_{n=1}^{∞}nx^{n-1}.
  3. The differentiated series still has radius 1, and its terms fail to approach zero at either endpoint.

Final answer

∑n=1∞nxn-1=1/(1-x)2∑_{n=1}^{∞}nx^{n-1}=1/(1-x)^2, for |x|<1|x|<1.

Problem 13

Added problem and worked solution

Integrate ∑n=0∞xn∑_{n=0}^{∞}x^n from 0 to x and state the resulting function and interval.

  1. Integrate the geometric series from 0 to x inside |x|<1|x|<1.
  2. This gives -ln(1-x)=∑n=0∞xn+1/(n+1)-ln(1-x)=∑_{n=0}^{∞}x^{n+1}/(n+1).
  3. The resulting series converges at x=−1 by the alternating test but diverges at x=1. Thus its interval is -1≤x<1-1≤x<1.

Final answer

-ln(1-x)=∑n=1∞xn/n-ln(1-x)=∑_{n=1}^{∞}x^n/n, for -1≤x<1-1≤x<1.

Problem 14

Added problem and worked solution

Find the cubic Taylor polynomial for exe^x centered at 1.

  1. For f(x)=exf(x)=e^x, every derivative at x=1 equals e.
  2. Insert those values in P3(x)=∑n=03f(n)(1)(x-1)n/n!P_3(x)=∑_{n=0}^{3}f^{(n)}(1)(x-1)^n/n!.

Final answer

P3(x)=e(1+(x-1)+(x-1)2/2+(x-1)3/6)P_3(x)=e(1+(x-1)+(x-1)^2/2+(x-1)^3/6).

Problem 15

Added problem and worked solution

Find the cubic Taylor polynomial of lnxln x centered at 2.

  1. For f(x)=lnxf(x)=ln x, the first four derivative values at 2 are f(2)=ln2f(2)=ln2, f′(2)=1/2f′(2)=1/2, f″(2)=-1/4f″(2)=-1/4, and f‴(2)=1/4f‴(2)=1/4.
  2. Divide the second and third derivative values by 2! and 3!, respectively, in the Taylor formula.

Final answer

P3(x)=ln2+(x-2)/2-(x-2)2/8+(x-2)3/24P_3(x)=ln2+(x-2)/2-(x-2)^2/8+(x-2)^3/24.

Problem 16

Added problem and worked solution

Taylor expand x3x^3 centered at 1.

  1. Set h=x-1h=x-1, so x3=(1+h)3x^3=(1+h)^3.
  2. The binomial theorem gives 1+3h+3h2+h31+3h+3h^2+h^3. There are no higher terms.

Final answer

x3=1+3(x-1)+3(x-1)2+(x-1)3x^3=1+3(x-1)+3(x-1)^2+(x-1)^3.

Problem 17

Added problem and worked solution

Taylor expand 1/x1/x centered at 2 and state where the series converges.

  1. Write x=2+hx=2+h. Then 1/x=(1/2)/(1+h/2)1/x=(1/2)/(1+h/2).
  2. Use the geometric series with ratio -h/2-h/2. The answer is ∑n=0∞(-1)n(x-2)n/2n+1∑_{n=0}^{∞}(-1)^n(x-2)^n/2^{n+1}.
  3. The series converges when |x-2|<2|x-2|<2. At either endpoint its terms fail to tend to zero.

Final answer

1/x=∑n=0∞(-1)n(x-2)n/2n+11/x=∑_{n=0}^{∞}(-1)^n(x-2)^n/2^{n+1}, for 0<x<40<x<4.

Problem 18

Added problem and worked solution

Taylor expand sinxsin x centered at π/2π/2.

  1. Set h=x-π/2h=x-π/2. The angle-addition identity gives sin(π/2+h)=coshsin(π/2+h)=cos h.
  2. Substitute the cosine Maclaurin series to get ∑n=0∞(-1)n(x-π/2)2n/(2n)!∑_{n=0}^{∞}(-1)^n(x-π/2)^{2n}/(2n)!. It converges for every real x.

Final answer

sinx=∑n=0∞(-1)n(x-π/2)2n/(2n)!sin x=∑_{n=0}^{∞}(-1)^n(x-π/2)^{2n}/(2n)!.

Problem 19

Added problem and worked solution

A Taylor series starts 5-2(x-3)+4(x-3)2+…5-2(x-3)+4(x-3)^2+…. Find f′(3)f′(3) and f″(3)f″(3).

  1. In a Taylor series centered at 3, the coefficient of (x-3)n(x-3)^n equals f(n)(3)/n!f^{(n)}(3)/n!.
  2. The linear coefficient gives f′(3)=-2f′(3)=-2. The quadratic coefficient 4 gives f″(3)=2!·4=8f″(3)=2!·4=8.

Final answer

f′(3)=-2f′(3)=-2 and f″(3)=8f″(3)=8.

Problem 20

Added problem and worked solution

Use the cubic Maclaurin polynomial to approximate e0.1e^{0.1} and bound the error with Taylor’s theorem.

  1. The cubic Taylor polynomial for exe^x at zero is 1+x+x2/2+x3/61+x+x^2/2+x^3/6.
  2. On 0≤x≤0.10≤x≤0.1, its fourth derivative is ex≤e0.1e^x≤e^{0.1}. Taylor’s remainder bound is |R3(0.1)|≤e0.1(0.1)4/4!|R_3(0.1)|≤e^{0.1}(0.1)^4/4!.
  3. Evaluating the bound gives approximately 0.0000046050.000004605, while the polynomial value is 1.1051666671.105166667.

Final answer

Approximation 1.1051666671.105166667, with error at most 0.0000046050.000004605.

Problem 21

Added problem and worked solution

How is a Maclaurin series related to a Taylor series?

  1. A Taylor series uses derivative values at its center c.
  2. Choosing c=0c=0 gives ∑n=0∞f(n)(0)xn/n!∑_{n=0}^{∞}f^{(n)}(0)x^n/n!, which is called the Maclaurin series.

Final answer

A Maclaurin series is a Taylor series centered at zero.

Problem 22

Added problem and worked solution

Find the Maclaurin series for e2xe^{2x} and its interval of convergence.

  1. Start from eu=∑n=0∞un/n!e^u=∑_{n=0}^{∞}u^n/n!.
  2. Substitute u=2xu=2x to obtain e2x=∑n=0∞2nxn/n!e^{2x}=∑_{n=0}^{∞}2^n x^n/n!. The exponential series converges for every real u, hence every real x.

Final answer

e2x=∑n=0∞2nxn/n!e^{2x}=∑_{n=0}^{∞}2^n x^n/n!.

Problem 23

Added problem and worked solution

Find the Maclaurin series for cos(3x)cos(3x).

  1. Use cosu=∑n=0∞(-1)nu2n/(2n)!cos u=∑_{n=0}^{∞}(-1)^n u^{2n}/(2n)!.
  2. Set u=3xu=3x, giving 1-9x2/2!+81x4/4!-729x6/6!+…1-9x^2/2!+81x^4/4!-729x^6/6!+…. The series converges for all real x.

Final answer

cos3x=∑n=0∞(-1)n32nx2n/(2n)!cos3x=∑_{n=0}^{∞}(-1)^n3^{2n}x^{2n}/(2n)!.

Problem 24

Added problem and worked solution

Find the Maclaurin series and interval of convergence of ln(1+2x)ln(1+2x).

  1. Start with ln(1+u)=∑n=1∞(-1)n+1un/nln(1+u)=∑_{n=1}^{∞}(-1)^{n+1}u^n/n for -1<u≤1-1<u≤1.
  2. Substitute u=2xu=2x. This yields ∑n=1∞(-1)n+12nxn/n∑_{n=1}^{∞}(-1)^{n+1}2^n x^n/n.
  3. At x=1/2x=1/2 the alternating harmonic series converges; at x=-1/2x=-1/2 the magnitude harmonic series diverges.

Final answer

ln(1+2x)=∑n=1∞(-1)n+12nxn/nln(1+2x)=∑_{n=1}^{∞}(-1)^{n+1}2^n x^n/n, for -1/2<x≤1/2-1/2<x≤1/2.

Problem 25

Added problem and worked solution

Give the first three nonzero terms of the Maclaurin series of sin(x2)sin(x^2).

  1. Substitute u=x2u=x^2 into sinu=u-u3/3!+u5/5!-…sin u=u-u^3/3!+u^5/5!-….
  2. The first three nonzero terms are x2-x6/6+x10/120x^2-x^6/6+x^{10}/120. The full series has infinite radius.

Final answer

sin(x2)=x2-x6/6+x10/120+…sin(x^2)=x^2-x^6/6+x^{10}/120+….

Problem 26

Added problem and worked solution

Find the cubic Maclaurin polynomial of exsinxe^x sin x.

  1. Use ex=1+x+x2/2+x3/6+…e^x=1+x+x^2/2+x^3/6+… and sinx=x-x3/6+…sin x=x-x^3/6+….
  2. Collect terms through degree 3: the x coefficient is 1, the x² coefficient is 1, and the x³ coefficient is 1/2-1/6=1/31/2-1/6=1/3.

Final answer

P3(x)=x+x2+x3/3P_3(x)=x+x^2+x^3/3.

Problem 27

Added problem and worked solution

Find the Maclaurin series of 1/(1+x2)1/(1+x^2) and its interval of convergence.

  1. The geometric formula 1/(1-u)=∑n=0∞un1/(1-u)=∑_{n=0}^{∞}u^n applies when |u|<1|u|<1.
  2. Set u=-x2u=-x^2, obtaining 1/(1+x2)=∑n=0∞(-1)nx2n1/(1+x^2)=∑_{n=0}^{∞}(-1)^n x^{2n}.
  3. At x=±1 the terms alternate ±1 and fail to tend to zero. The interval is (-1,1)(-1,1).

Final answer

1-x2+x4-x6+…1-x^2+x^4-x^6+…, for |x|<1|x|<1.

Problem 28

Added problem and worked solution

What is the coefficient of x⁵ in the Maclaurin series for x2exx^2e^x?

  1. Multiplying ex=∑xn/n!e^x=∑x^n/n! by x² gives x2ex=∑xn+2/n!x^2e^x=∑x^{n+2}/n!.
  2. The x⁵ term requires n+2=5n+2=5, hence n=3. Its coefficient is 1/3!=1/61/3!=1/6.

Final answer

1/61/6.

Problem 29

Added problem and worked solution

Must a Taylor series represent its function at every point in the function’s domain? Give a concrete example.

  1. The Maclaurin expansion of 1/(1-x)1/(1-x) is the geometric series ∑xn∑x^n, whose radius is 1.
  2. The function itself exists for every x≠1x≠1, but the series diverges when |x|≥1|x|≥1. A function’s domain can therefore exceed the convergence interval of one Taylor expansion.

Final answer

No; 1/(1-x)1/(1-x) exists at x=2, but its Maclaurin series diverges there.

Problem 30

Added problem and worked solution

Find the quadratic Maclaurin polynomial for sqrt(1+x)sqrt(1+x).

  1. For f(x)=sqrt(1+x)f(x)=sqrt(1+x), f(0)=1f(0)=1, f′(0)=1/2f′(0)=1/2, and f″(0)=-1/4f″(0)=-1/4.
  2. Divide the second derivative by 2! in the Taylor formula. This gives the quadratic Maclaurin polynomial 1+x/2-x2/81+x/2-x^2/8.

Final answer

P2(x)=1+x/2-x2/8P_2(x)=1+x/2-x^2/8.

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