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5.4E: Exercises for Section 5.4

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In exercises 1 - 4, use appropriate substitutions to write down the Maclaurin series for the given binomial.

1) (1x)1/3

2) (1+x2)1/3

Answer
(1+x2)1/3=n=0(n13)x2n

3) (1x)1.01

4) (12x)2/3

Answer
(12x)2/3=n=0(1)n2n(n23)xn

In exercises 5 - 12, use the substitution (b+x)r=(b+a)r(1+xab+a)r in the binomial expansion to find the Taylor series of each function with the given center.

5) x+2 at a=0

6) x2+2 at a=0

Answer
2+x2=n=02(1/2)n(n12)x2n;(|x2|<2)

7) x+2 at a=1

8) 2xx2 at a=1 (Hint: 2xx2=1(x1)2)

Answer
2xx2=1(x1)2 so 2xx2=n=0(1)n(n12)(x1)2n

9) (x8)1/3 at a=9

10) x at a=4

Answer
x=21+x44 so x=n=0212n(n12)(x4)n

11) x1/3 at a=27

12) x at x=9

Answer
x=n=0313n(n12)(x9)n

In exercises 13 - 14, use the binomial theorem to estimate each number, computing enough terms to obtain an estimate accurate to an error of at most 1/1000.

13) [T] (15)1/4 using (16x)1/4

14) [T] (1001)1/3 using (1000+x)1/3

Answer
10(1+x1000)1/3=n=01013n(13n)xn. Using, for example, a fourth-degree estimate at x=1 gives (1001)1/310(1+(113)103+(213)106+(313)109+(313)1012)=10(1+13.10319.106+581.10910243.1012)=10.00333222... whereas (1001)1/3=10.00332222839093.... Two terms would suffice for three-digit accuracy.

In exercises 15 - 18, use the binomial approximation 1x1x2x28x3165x41287x5256 for |x|<1 to approximate each number. Compare this value to the value given by a scientific calculator.

15) [T] 12 using x=12 in (1x)1/2

16) [T] 5=5×15 using x=45 in (1x)1/2

Answer
The approximation is 2.3152; the CAS value is 2.23.

17) [T] 3=33 using x=23 in (1x)1/2

18) [T] 6 using x=56 in (1x)1/2

Answer
The approximation is 2.583; the CAS value is 2.449.

19) Integrate the binomial approximation of 1x to find an approximation of x01tdt.

20) [T] Recall that the graph of 1x2 is an upper semicircle of radius 1. Integrate the binomial approximation of 1x2 up to order 8 from x=1 to x=1 to estimate π2.

Answer
1x2=1x22x48x6165x8128+. Thus 111x2dx=[xx36x540x77165x99128+]|11213120156109128+error=1.590... whereas π2=1.570...

In exercises 21 - 24, use the expansion (1+x)1/3=1+13x19x2+581x310243x4+ to write the first five terms (not necessarily a quartic polynomial) of each expression.

21) (1+4x)1/3;a=0

22) (1+4x)4/3;a=0

Answer
(1+x)4/3=(1+x)(1+13x19x2+581x310243x4+)=1+4x3+2x294x381+5x4243+

23) (3+2x)1/3;a=1

24) (x2+6x+10)1/3;a=3

Answer
(1+(x+3)2)1/3=1+13(x+3)219(x+3)4+581(x+3)610243(x+3)8+

25) Use (1+x)1/3=1+13x19x2+581x310243x4+ with x=1 to approximate 21/3.

26) Use the approximation (1x)2/3=12x3x294x3817x424314x5729+ for |x|<1 to approximate 21/3=2.22/3.

Answer
Twice the approximation is 1.260 whereas 21/3=1.2599....

27) Find the 25th derivative of f(x)=(1+x2)13 at x=0.

28) Find the 99th derivative of f(x)=(1+x4)25.

Answer
f(99)(0)=0

In exercises 29 - 36, find the Maclaurin series of each function.

29) f(x)=xe2x

30) f(x)=2x

Answer
n=0(ln(2)x)nn!

31) f(x)=sinxx

32) f(x)=sin(x)x,(x>0),

Answer
For x>0,sin(x)=n=0(1)nx(2n+1)/2x(2n+1)!=n=0(1)nxn(2n+1)!.

33) f(x)=sin(x2)

34) f(x)=ex3

Answer
ex3=n=0x3nn!

35) f(x)=cos2x using the identity cos2x=12+12cos(2x)

36) f(x)=sin2x using the identity sin2x=1212cos(2x)

Answer
sin2x=k=1(1)k22k1x2k(2k)!

In exercises 37 - 44, find the Maclaurin series of F(x)=x0f(t)dt by integrating the Maclaurin series of f term by term. If f is not strictly defined at zero, you may substitute the value of the Maclaurin series at zero.

37) F(x)=x0et2dt;f(t)=et2=n=0(1)nt2nn!

38) F(x)=tan1x;f(t)=11+t2=n=0(1)nt2n

Answer
tan1x=k=0(1)kx2k+12k+1

39) F(x)=tanh1x;f(t)=11t2=n=0t2n

40) F(x)=sin1x;f(t)=11t2=k=0(k12)t2kk!

Answer
sin1x=n=0(n12)x2n+1(2n+1)n!

41) F(x)=x0sinttdt;f(t)=sintt=n=0(1)nt2n(2n+1)!

42) F(x)=x0cos(t)dt;f(t)=n=0(1)nxn(2n)!

Answer
F(x)=n=0(1)nxn+1(n+1)(2n)!

43) F(x)=x01costt2dt;f(t)=1costt2=n=0(1)nt2n(2n+2)!

44) F(x)=x0ln(1+t)tdt;f(t)=n=0(1)ntnn+1

Answer
F(x)=n=1(1)n+1xnn2

In exercises 45 - 52, compute at least the first three nonzero terms (not necessarily a quadratic polynomial) of the Maclaurin series of f.

45) f(x)=sin(x+π4)=sinxcos(π4)+cosxsin(π4)

46) f(x)=tanx

Answer
x+x33+2x515+

47) f(x)=ln(cosx)

48) f(x)=excosx

Answer
1+xx33x46+

49) f(x)=esinx

50) f(x)=sec2x

Answer
1+x2+2x43+17x645+

51) f(x)=tanhx

52) f(x)=tanxx (see expansion for tanx)

Answer
Using the expansion for tanx gives 1+x3+2x215.

In exercises 53 - 56, find the radius of convergence of the Maclaurin series of each function.

53) ln(1+x)

54) 11+x2

Answer
11+x2=n=0(1)nx2n so R=1 by the ratio test.

55) tan1x

56) ln(1+x2)

Answer
ln(1+x2)=n=1(1)n1nx2n so R=1 by the ratio test.

57) Find the Maclaurin series of sinhx=exex2.

58) Find the Maclaurin series of coshx=ex+ex2.

Answer
Add series of ex and ex term by term. Odd terms cancel and coshx=n=0x2n(2n)!.

59) Differentiate term by term the Maclaurin series of sinhx and compare the result with the Maclaurin series of coshx.

60) [T] Let Sn(x)=nk=0(1)kx2k+1(2k+1)! and Cn(x)=nn=0(1)kx2k(2k)! denote the respective Maclaurin polynomials of degree 2n+1 of sinx and degree 2n of cosx. Plot the errors Sn(x)Cn(x)tanx for n=1,..,5 and compare them to x+x33+2x515+17x7315tanx on (π4,π4).

Answer

The ratio Sn(x)Cn(x) approximates tanx better than does p7(x)=x+x33+2x515+17x7315 for N3. The dashed curves are SnCntanx for n=1,2. The dotted curve corresponds to n=3, and the dash-dotted curve corresponds to n=4. The solid curve is p7tanx.

This graph has two curves. The first one is a decreasing function passing through the origin. The second is a broken line which is an increasing function passing through the origin. The two curves are very close around the origin.

61) Use the identity 2sinxcosx=sin(2x) to find the power series expansion of sin2x at x=0. (Hint: Integrate the Maclaurin series of sin(2x) term by term.)

62) If y=n=0anxn, find the power series expansions of xy and x2y.

Answer
By the term-by-term differentiation theorem, \displaystyle y′=\sum_{n=1}^∞na_nx^{n−1} so \displaystyle y′=\sum_{n=1}^∞na_nx^{n−1}xy′=\sum_{n=1}^∞na_nx^n, whereas \displaystyle y′=\sum_{n=2}^∞n(n−1)a_nx^{n−2} so \displaystyle xy''=\sum_{n=2}^∞n(n−1)a_nx^n.

63) [T] Suppose that \displaystyle y=\sum_{k=0}^∞a^kx^k satisfies y′=−2xy and y(0)=0. Show that a_{2k+1}=0 for all k and that a_{2k+2}=\dfrac{−a_{2k}}{k+1}. Plot the partial sum S_{20} of y on the interval [−4,4].

64) [T] Suppose that a set of standardized test scores is normally distributed with mean μ=100 and standard deviation σ=10. Set up an integral that represents the probability that a test score will be between 90 and 110 and use the integral of the degree 10 Maclaurin polynomial of \frac{1}{\sqrt{2π}}e^{−x^2/2} to estimate this probability.

Answer
The probability is \displaystyle p=\frac{1}{\sqrt{2π}}∫^{(b−μ)/σ}_{(a−μ)/σ}e^{−x^2/2}\,dx where a=90 and b=100, that is, \displaystyle p=\frac{1}{\sqrt{2π}}∫^1_{−1}e^{−x^2/2}\,dx=\frac{1}{\sqrt{2π}}∫^1_{−1}\sum_{n=0}^5(−1)^n\frac{x^{2n}}{2^nn!}\,dx=\frac{2}{\sqrt{2π}}\sum_{n=0}^5(−1)^n\frac{1}{(2n+1)2^nn!}≈0.6827.

65) [T] Suppose that a set of standardized test scores is normally distributed with mean μ=100 and standard deviation σ=10. Set up an integral that represents the probability that a test score will be between 70 and 130 and use the integral of the degree 50 Maclaurin polynomial of \frac{1}{\sqrt{2π}}e^{−x^2/2} to estimate this probability.

66) [T] Suppose that \displaystyle \sum_{n=0}^∞a_nx^n converges to a function f(x) such that f(0)=1,\, f′(0)=0, and f''(x)=−f(x). Find a formula for a_n and plot the partial sum S_N for N=20 on [−5,5].

Answer

As in the previous problem one obtains a_n=0 if n is odd and a_n=−(n+2)(n+1)a_{n+2} if n is even, so a_0=1 leads to a_{2n}=\dfrac{(−1)^n}{(2n)!}.

This graph is a wave curve symmetrical about the origin. It has a peak at y = 1 above the origin. It has lowest points at -3 and 3.

67) [T] Suppose that \displaystyle \sum_{n=0}^∞a_nx^n converges to a function f(x) such that f(0)=0,\; f′(0)=1, and f''(x)=−f(x). Find a formula for an and plot the partial sum S_N for N=10 on [−5,5].

68) Suppose that \displaystyle \sum_{n=0}^∞a_nx^n converges to a function y such that y''−y′+y=0 where y(0)=1 and y'(0)=0. Find a formula that relates a_{n+2},\;a_{n+1}, and an and compute a_0,...,a_5.

Answer
\displaystyle y''=\sum_{n=0}^∞(n+2)(n+1)a_{n+2}x^n and \displaystyle y′=\sum_{n=0}^∞(n+1)a_{n+1}x^n so y''−y′+y=0 implies that (n+2)(n+1)a_{n+2}−(n+1)a_{n+1}+a_n=0 or a_n=\dfrac{a_{n−1}}{n}−\dfrac{a_{n−2}}{n(n−1)} for all n⋅y(0)=a_0=1 and y′(0)=a_1=0, so a_2=\frac{1}{2},\;a_3=\frac{1}{6}\;,a_4=0, and a_5=−\frac{1}{120}.

69) Suppose that \displaystyle \sum_{n=0}^∞a_nx^n converges to a function y such that y''−y′+y=0 where y(0)=0 and y′(0)=1. Find a formula that relates a_{n+2},\;a_{n+1}, and an and compute a_1,...,a_5.

The error in approximating the integral \displaystyle ∫^b_af(t)\, dt by that of a Taylor approximation \displaystyle ∫^b_aPn(t) \,dt is at most \displaystyle ∫^b_aR_n(t) \,dt. In exercises 70 - 71, the Taylor remainder estimate R_n≤\frac{M}{(n+1)!}|x−a|^{n+1} guarantees that the integral of the Taylor polynomial of the given order approximates the integral of f with an error less than \frac{1}{10}.

a. Evaluate the integral of the appropriate Taylor polynomial and verify that it approximates the CAS value with an error less than \frac{1}{100}.

b. Compare the accuracy of the polynomial integral estimate with the remainder estimate.

70) [T] \displaystyle ∫^π_0\frac{\sin t}{t}\, dt;\quad P_s=1−\frac{x^2}{3!}+\frac{x^4}{5!}−\frac{x^6}{7!}+\frac{x^8}{9!} (You may assume that the absolute value of the ninth derivative of \frac{\sin t}{t} is bounded by 0.1.)

Answer
a. (Proof)
b. We have R_s≤\frac{0.1}{(9)!}π^9≈0.0082<0.01. We have \displaystyle ∫^π_0\left(1−\frac{x^2}{3!}+\frac{x^4}{5!}−\frac{x^6}{7!}+\frac{x^8}{9!}\right)\,dx=π−\frac{π^3}{3⋅3!}+\frac{π^5}{5⋅5!}−\frac{π^7}{7⋅7!}+\frac{π^9}{9⋅9!}=1.852..., whereas \displaystyle ∫^π_0\frac{\sin t}{t}\,dt=1.85194..., so the actual error is approximately 0.00006.

71) [T] \displaystyle ∫^2_0e^{−x^2}\,dx;\; p_{11}=1−x^2+\frac{x^4}{2}−\frac{x^6}{3!}+⋯−\frac{x^{22}}{11!} (You may assume that the absolute value of the 23^{\text{rd}} derivative of e^{−x^2} is less than 2×10^{14}.)

The following exercises (72-73) deal with Fresnel integrals.

72) The Fresnel integrals are defined by \displaystyle C(x)=∫^x_0\cos(t^2)\,dt and \displaystyle S(x)=∫^x_0\sin(t^2)\,dt. Compute the power series of C(x) and S(x) and plot the sums C_N(x) and S_N(x) of the first N=50 nonzero terms on [0,2π].

Answer

Since \displaystyle \cos(t^2)=\sum_{n=0}^∞(−1)^n\frac{t^{4n}}{(2n)!} and \displaystyle \sin(t^2)=\sum_{n=0}^∞(−1)^n\frac{t^{4n+2}}{(2n+1)!}, one has \displaystyle S(x)=\sum_{n=0}^∞(−1)^n\frac{x^{4n+3}}{(4n+3)(2n+1)!} and \displaystyle C(x)=\sum_{n=0}^∞(−1)^n\frac{x^{4n+1}}{(4n+1)(2n)!}. The sums of the first 50 nonzero terms are plotted below with C_{50}(x) the solid curve and S_{50}(x) the dashed curve.

This graph has two curves. The first one is a solid curve labeled Csub50(x). It begins at the origin and is a wave that gradually decreases in amplitude. The highest it reaches is y = 1. The second curve is labeled Ssub50(x). It is a wave that gradually decreases in amplitude. The highest it reaches is 0.9. It is very close to the pattern of the first curve with a slight shift to the right.

73) [T] The Fresnel integrals are used in design applications for roadways and railways and other applications because of the curvature properties of the curve with coordinates (C(t),S(t)). Plot the curve (C_{50},S_{50}) for 0≤t≤2π, the coordinates of which were computed in the previous exercise.

74) Estimate \displaystyle ∫^{1/4}_0\sqrt{x−x^2}\,dx by approximating \sqrt{1−x} using the binomial approximation \displaystyle 1−\frac{x}{2}−\frac{x^2}{8}−\frac{x^3}{16}−\frac{5x^4}{2128}−\frac{7x^5}{256}.

Answer
\displaystyle ∫^{1/4}_0\sqrt{x}\left(1−\frac{x}{2}−\frac{x^2}{8}−\frac{x^3}{16}−\frac{5x^4}{128}−\frac{7x^5}{256}\right)\,dx =\frac{2}{3}2^{−3}−\frac{1}{2}\frac{2}{5}2^{−5}−\frac{1}{8}\frac{2}{7}2^{−7}−\frac{1}{16}\frac{2}{9}2^{−9}−\frac{5}{128}\frac{2}{11}2^{−11}−\frac{7}{256}\frac{2}{13}2^{−13}=0.0767732... whereas \displaystyle ∫^{1/4}_0\sqrt{x−x^2}\, dx=0.076773.

75) [T] Use Newton’s approximation of the binomial \sqrt{1−x^2} to approximate π as follows. The circle centered at (\frac{1}{2},0) with radius \frac{1}{2} has upper semicircle y=\sqrt{x}\sqrt{1−x}. The sector of this circle bounded by the x-axis between x=0 and x=\frac{1}{2} and by the line joining (\frac{1}{4},\frac{\sqrt{3}}{4}) corresponds to \frac{1}{6} of the circle and has area \frac{π}{24}. This sector is the union of a right triangle with height \frac{\sqrt{3}}{4} and base \frac{1}{4} and the region below the graph between x=0 and x=\frac{1}{4}. To find the area of this region you can write y=\sqrt{x}\sqrt{1−x}=\sqrt{x}×(\text{binomial expansion of} \sqrt{1−x}) and integrate term by term. Use this approach with the binomial approximation from the previous exercise to estimate π.

76) Use the approximation T≈2π\sqrt{\frac{L}{g}}(1+\frac{k^2}{4}) to approximate the period of a pendulum having length 10 meters and maximum angle θ_{max}=\frac{π}{6} where k=\sin\left(\frac{θ_{max}}{2}\right). Compare this with the small angle estimate T≈2π\sqrt{\frac{L}{g}}.

Answer
T≈2π\sqrt{\frac{10}{9.8}}\left(1+\frac{\sin^2(θ/12)}{4}\right)≈6.453 seconds. The small angle estimate is T≈2π\sqrt{\frac{10}{9.8}≈6.347}. The relative error is around 2 percent.

77) Suppose that a pendulum is to have a period of 2 seconds and a maximum angle of θ_{max}=\frac{π}{6}. Use T≈2π\sqrt{\dfrac{L}{g}}\left(1+\dfrac{k^2}{4}\right) to approximate the desired length of the pendulum. What length is predicted by the small angle estimate T≈2π\sqrt{\frac{L}{g}}?

78) Evaluate \displaystyle ∫^{π/2}_0\sin^4θ\,dθ in the approximation \displaystyle T=4\sqrt{\frac{L}{g}}∫^{π/2}_0\left(1+\frac{1}{2}k^2\sin^2θ+\frac{3}{8}k^4\sin^4θ+⋯\right)\,dθ to obtain an improved estimate for T.

Answer
\displaystyle ∫^{π/2}_0\sin^4θ\, dθ=\frac{3π}{16}. Hence T≈2π\sqrt{\frac{L}{g}}\left(1+\frac{k^2}{4}+\frac{9}{256}k^4\right).

79) [T] An equivalent formula for the period of a pendulum with amplitude \displaystyle θ_{max} is T(θ_{max})=2\sqrt{2}\sqrt{\frac{L}{g}}∫^{θ_{max}}_0\frac{dθ}{\sqrt{\cos θ}−\cos(θ_{max})} where L is the pendulum length and g is the gravitational acceleration constant. When θ_{max}=\frac{π}{3} we get \dfrac{1}{\sqrt{\cos t−1/2}}≈\sqrt{2}\left(1+\frac{t^2}{2}+\frac{t^4}{3}+\frac{181t^6}{720}\right). Integrate this approximation to estimate T(\frac{π}{3}) in terms of L and g. Assuming g=9.806 meters per second squared, find an approximate length L such that T(\frac{π}{3})=2 seconds.

Contributors

Gilbert Strang (MIT) and Edwin “Jed” Herman (Harvey Mudd) with many contributing authors. This content by OpenStax is licensed with a CC-BY-SA-NC 4.0 license. Download for free at http://cnx.org.


This page titled 5.4E: Exercises for Section 5.4 is shared under a CC BY-NC-SA 4.0 license and was authored, remixed, and/or curated by OpenStax via source content that was edited to the style and standards of the LibreTexts platform.

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