Answers
- a) ln(1+x)=∑n=1∞(−1)n+1nxn, constant ln1=0
- b) Interval (−1,1]: the endpoint 1 is gained; 1−21+31−⋯=ln2.
- c) arctanx=∑n=0∞(−1)n2n+1x2n+1 on [−1,1]; 1−31+51−⋯=4π
- d) ln(5−x)=ln5−∑n=1∞n5nxn, interval [−5,5)
- e) ∑n=0∞(4n+1)24n+1(−1)n; 21−1601+46081=2304011381, error below 1064961
a) On (−1,1), 1+t1=1−(−t)1=∑n=0∞(−1)ntn. For ∣x∣<1 the interval [0,x] lies inside the interval of convergence, so the series can be integrated term by term on it: ln(1+x)=∫0x1+tdt=∑n=0∞(−1)nn+1xn+1=∑n=1∞(−1)n+1nxn=x−2x2+3x3−⋯. The definite integral from 0 fixes the constant by itself. With an indefinite integral one writes ln(1+x)=C+∑(⋯) and finds C at the centre: ln1=C+0, so C=0. The constant is 0 here only because ln(1+0)=0; d) shows a case where it is not.
b) Radius 1 by the theorem (or by the ratio test: n+1n∣x∣→∣x∣). At x=1: ∑n(−1)n+1, the alternating harmonic series, converges by the alternating series test, since n1 decreases to 0. At x=−1: (−1)n+1(−1)n=−1, so the series is −∑n1, which diverges. Interval: (−1,1]. The series of 1+x1 had interval (−1,1): integrating kept R and GAINED the endpoint x=1. Since ln(1+x) is continuous at 1 and the series converges there, Abel's theorem gives 1−21+31−41+⋯=ln2. Beyond x=1, the figure shows S5 and S6 leaving ln(1+x) in opposite directions: for x>1 the terms nxn grow without bound, and the series represents nothing there, although ln(1+x) exists. Near x=−1, ln(1+x)→−∞ while every partial sum stays finite: the divergence at −1 is visible as well.
c) 1+t21=∑n=0∞(−1)nt2n for ∣t∣<1 (Exercise 4). Integrate from 0 to x: arctanx=∑n=0∞(−1)n2n+1x2n+1=x−3x3+5x5−⋯, with constant arctan0=0. At x=1: ∑2n+1(−1)n, alternating with 2n+11 decreasing to 0, converges. At x=−1: (−1)2n+1=−1, so the series is −∑2n+1(−1)n, which converges as well. Interval [−1,1]: BOTH endpoints are gained, where 1+x21 had (−1,1). Both converge only conditionally, since ∑2n+11 diverges by limit comparison with ∑n1. Abel's theorem at x=1: 1−31+51−71+⋯=arctan1=4π.
d) Differentiate first: dxdln(5−x)=−5−x1=−51⋅1−5x1=−∑n=0∞5n+1xn for ∣x∣<5. Integrate term by term: ln(5−x)=C−∑n=0∞(n+1)5n+1xn+1=C−∑n=1∞n5nxn. At the centre x=0: ln5=C−0, so C=ln5 and ln(5−x)=ln5−∑n=1∞n5nxn. Forgetting C gives a series worth 0 at x=0 where the function is worth ln5: the check at the centre catches it in one line. Endpoints: at x=5, ∑n1 diverges (and indeed ln(5−x)→−∞ as x→5−); at x=−5, ∑n(−1)n converges by the alternating series test. Interval: [−5,5).
e) For ∣x∣<1, 1+x41=∑n=0∞(−1)nx4n (u=−x4). The interval of integration [0,21] lies inside (−1,1), so term-by-term integration is justified: ∫01/21+x4dx=∑n=0∞(−1)n[4n+1x4n+1]01/2=∑n=0∞(4n+1)24n+1(−1)n=21−1601+46081−1064961+⋯. This numerical series is alternating with bn=(4n+1)24n+11 decreasing to 0, so by the alternating series estimate the error after three terms is at most the fourth, 13⋅2131=1064961<10−5. The approximation, over the common denominator 23040=29⋅45: 21−1601+46081=2304011520−144+5=2304011381, about 0.4940. The function has an elementary antiderivative, but it needs a four-factor partial fraction decomposition; the series gives the value to 10−5 in three lines.