Comments
Description
Transcript
Mathematical Series
Chapter 10 Mathematical Series EXERCISES Exercise 10.1. Show that in the series of Eq. (10.4) any term of the series is equal to the sum of all the terms following it. ( Hint: Factor a factor out of all of the following terms so that they will equal this factor times the original series, whose value is now known.) Let the given term be denoted by term = b. 0.001%. 0.001% of 1.64993 is equal to 0.00016449. The n = 79 term is equal to 0.0001602, so we need the partial sum S79 . However, this partial sum is equal to 1.6324, so again this approximation does not work very well. Exercise 10.3. Find the value of the infinite series 1 2n ∞ The following terms are [ln (2)]n n=0 1 1 1 1 + n+2 + n+3 + n+4 + · · · 2n+1 2 2 2 1 1 1 1 1 = n+1 1 + + + + · · · + n + · · · 2 2 4 8 2 1 2 = n+1 = n 2 2 Exercise 10.2. Consider the series s =1+ 1 1 1 1 + 2 + 2 + ··· + 2 + ··· 22 3 4 n which is known to be convergent and to equal π 2 6/ = 1.64993 · · ·. Using Eq. (10.5) as an approximation, determine which partial sum approximates the series to a. 1% 1% of 1.64993 is equal to 0.016449. The n = 8 term is equal to 0.015625, so we need the partial sum S8 , which is equal to 1.2574· · ·. The series is slowly convergent and S8 is equal to 1.5274, so this approximation does not work very well. Mathematics for Physical Chemistry. http://dx.doi.org/10.1016/B978-0-12-415809-2.00056-2 © 2013 Elsevier Inc. All rights reserved. Determine how well this series is approximated by S2 ,S5 , and S10 . This is a geometric series, so the sum is s= 1 = 3.25889 · · · 1 − ln (2) The partial sums are S2 = 1 + ln (2) = 1.693 · · · S5 = 1 + ln (2) + ln (2)2 + ln (2)3 + ln (2)4 = 2.73746 · · · S10 = 3.175461 S20 = 3.256755 · · · Exercise 10.4. Evaluate the first 20 partial sums of the harmonic series. e57 e58 Mathematics for Physical Chemistry Here are the first 20 partial sums, obtained with Excel: ' Exercise 10.7. Show that the Maclaurin series for e x is $ ex = 1 + 1 1 1 1 1 x + x2 + x3 + x4 + · · · 1! 2! 3! 4! Every derivative of e x is equal to e x 1 dn f 1 an = = n! dx n x=0 n! 1.5 1.833333333 2.083333333 2.283333333 Exercise 10.8. Find the Maclaurin series for ln (1 + x). You can save some work by using the result of the previous example. The series is 2.45 2.592857143 2.717857143 2.828968254 ln (1 + x) = a0 + a1 x + a2 x 2 + · · · 2.928968254 3.019877345 3.103210678 d f dx 3.180133755 3.251562327 The second derivative is d2 f 1 = −1 = −1 2 dx 2 x=0 1 + x x=0 3.318228993 3.380728993 3.439552523 3.495108078 3.547739657 3.597739657 & a0 = ln (1) = 0 1 = =1 1 + x x=0 x=0 % Exercise 10.5. Show that the geometric series converges if r 2 ≺ 1. If r is positive, we apply the ratio test: an+1 lim =r n→∞ an If r 2 ≺ 1 and if r is positive, then r ≺ 1, so the series converges. If r is negative, apply the alternating series test. Each term is smaller than the previous term and approaches zero as you go further into the series, so the series converges. Exercise 10.6. Test the following series for convergence. ∞ 1 n2 n=1 Apply the ratio test: n2 1/(n + 1)2 r = lim = lim =1 n→∞ n→∞ (n + 1)2 1/n 2 The ratio test fails. We apply the integral text: ∞ ∞ 1 1 dx = − =1 2 x x 1 1 The integral converges, so the series converges. The derivatives follow a pattern: n n−1 d f n−1 (n − 1)! = (− 1) = −1 (n −1)! n n dx x=1 (1 + x) x=0 1 dn f (− 1)n−1 = n! dx n x=1 n The series is ln (1+x) = x− 1 1 1 1 x 2+ x 3− x 4+ x 5 +· · · 2 3 4 5 Exercise 10.9. Find the Taylor series for ln (x), expanding about x = 2, and show that the radius of convergence for this series is equal to 2, so that the series can represent the function in the region 0 ≺ x 4. The first term is determined by letting x = 2 in which case all of the terms except for a0 vanish: a0 = ln (2) The first derivative of ln (x) is 1/x, which equals 1/2 at x = 2. The second derivative is −1/x 2 , which equals −1/4 at x = 2. The third derivative is 2!/x 3 , which equals 1/4 at x = 1. The derivatives follow a regular pattern, n d f (n − 1)! n−1 (n − 1)! = (−1) = ( − 1)n−1 dx n x=2 x n x=2 2n so that 1 n! dn f dx n = x=1 (−1)n−1 n2n CHAPTER | 10 Mathematical Series and 1 1 ln (x) = ln (2) + (x − 2) − (x − 2)2 + (x − 2)3 8 24 1 − (x − 2)4 + · · · 64 The function is not analytic at x = 0, so the series is not valid at x = 0. For positive values of x the series is alternating, so we apply the alternating series test: (x − 2)n ( − 1)n−1 tn = an (x − 2)n = n2n 0 if|x − 2| ≺ 2 or 0 ≺ x 4 lim |tn | = n→∞ ∞ if|x − 2| > 2 or x > 4. Exercise 10.10. Find the series for 1/(1 − x), expanding about x = 0. What is the interval of convergence? 1 = a0 + a1 x + a2 x 2 + · · · 1+x a0 = 1 1 d 1 = − = −1 2 dx 1 + x x=0 (1 + x) x=0 1 1 1 d 2 − a2 = = =1 2 3 2! dx (1 + x) 2! (1 + x) x=0 x=0 a1 = The pattern continues: an = (−1)n 1 = 1 − x + x2 − x3 + x4 − x5 + · · · 1+x Since the function is not analytic at x = −1, the interval of convergence is −1 ≺ x ≺ 1 Exercise 10.11. Find the relationship between the coefficients A3 and B3 . We begin with the virial equation of state P= RT B2 RT B3 RT + + + ··· 2 Vm Vm Vm3 We write the pressure virial equation of state: RT A2 P A3 P 2 P= + + + ··· Vm Vm Vm We replace P and P 2 in this equation with the expression from the virial equation of state: A2 RT RT B2 RT B3 RT + + + + ··· P = Vm Vm Vm Vm2 Vm3 2 A3 RT RT B2 RT B3 + + + + · · · + ··· Vm Vm Vm2 Vm3 e59 We use the expression for the square of a power series from Eq. (5) of Appendix C, part 2: 2 RT B2 RT B3 RT + + + ··· Vm Vm2 Vm3 4 RT 2 RT RT B2 1 = +2 + O Vm Vm Vm2 Vm 4 2 2 1 RT 2 R T B2 +O = +2 3 Vm Vm Vm RT A2 RT RT B2 RT B3 P = + + + + ··· Vm Vm Vm Vm2 Vm3 2 2 4 R T B2 RT 2 1 A3 +2 +O + 3 Vm Vm Vm Vm RT RT A2 RT A2 B2 A3 RT 2 +··· = + + + Vm Vm2 Vm3 Vm Vm = RT B22 RT RT B2 A3 R 2 T 2 + + + 2 3 Vm Vm Vm Vm3 where we have replaced A2 by B2 . We now equation 2 coefficients of equal powers of 1/Vm in the two series for P: RT B3 = RT B22 + A3 R 2 T 2 A3 = B3 − RT B22 Exercise 10.12. Determine how large X 2 can be before the truncation of Eq. (10.28) that was used in Eq. (10.16) is inaccurate by more than 1%. 1 2 X + ··· 2 2 If the second term is smaller than 1% of the first term (which was the only one used in the approximation) the approximation should be adequate. By trial and error, we find that if X 2 = 0.019, the second term is equal to 0.0095 = 0.95% of the first term. − ln (X 1 ) = − ln (1 − X 2 ) = X 2 − Exercise 10.13. From the Maclaurin series for ln (1 + x) 1 1 ln (1 + x) = x − x 2 + x 3 + · · · 2 3 find the Taylor series for 1/(1 + x), using the fact that d[ln (1 + x)] 1 = . dx 1+x For what values of x is your series valid? 1 d 1 2 1 3 = x − x + x ··· 1+x dx 2 3 3x 2 4x 3 2x + − =1− 2 3 4 = 1 − x + x2 − x3 + x4 − x5 + · · · which is the series already obtained for 1/(1 + x) in an earlier example. The series is invalid if x 1. e60 Mathematics for Physical Chemistry Exercise 10.14. Find the formulas for the coefficients in a Taylor series that expands the function f (x,y) around the point x = a,y = b. f (x,y) = a00 + a10 (x − a) + a01 (y − b) + a11 (x − a) (y − b) + a21 (x − a)2 (y − b) + a12 (x − a) (y − b)2 + · · · a00 = f (a,b) ∂ f a10 = ∂ y x x=a,b=y ∂ f a01 = ∂ y x a,b 2 ∂ f a11 = ∂ y∂ x a,b n+m ∂ f 1 amn = m n n!m! ∂ y∂ x π π 2 + a2 x − sin (x) = a0 + a1 x − + ··· 4 4 where x is measured in radians. What is the radius of convergence of the series? PROBLEMS 1. Test the following series for convergence. (( − 1)n (n − 1)/n 2 ). n=0 We apply the alternating series test: n n−1 = lim limn→∞ |tn | = limn→∞ n→∞ n2 n2 1 =0 = limn→∞ n The series is convergent. 3. Test the following series for convergence. ∞ 1/n! . n=0 Try the ratio test an+1 n! 1 = lim =0 = lim n→∞ an n→∞ (n + 1)! n→∞ n + 1 The series converges. 5. Find the Taylor series for cos (x), expanding about x = π/2. r = lim cos (x)= a0 + a1 (x − π/2) + a2 (x − π/2)2 + · · · a0 = cos π/2 = 0 1 d 1 [cos (x)] a1 = = − sin (x) = −1 1! dx 2! π/2 π/2 1 d 1 [cos (x)] = − cos (x) =0 a2 = 2! dx 2! π/2 π/2 1 d 1 1 [cos (x)] sin (x) = = a3 = − 3! dx 3! 3! π/2 1 1 (x − π/2) + (x − π/2)3 1! 3! 1 − (x − π/2)5 + · · · 5! cos (x) = − 7. Find the coefficients of the first few terms of the Taylor series a,b ∞ There is a pattern, with all even-numbered coefficients vanishing and odd-numbered coefficients alternating between 1/n! and −1/n!. π/2 1 a0 = sin (π/4) = √ = 0.717107 2 1 1 cos (x) a1 = =√ 1! 2 π/4 1 1 =− √ a2 = − sin (x) 2! 2! 2 π/4 1 1 cos (x) = √ a3 = 3! 3! 2 π/4 The coefficients form a regular pattern: 1 √ n! 2 1 1 π π 2 1 + √ x− sin (x) = √ − √ x − 4 4 2 2 2! 2 n 1 π n π 3 1 − √ x− + · · · − −1 √ x− 4 4 3! 2 n! 2 +··· an = −(−1)n Since the function is analytic everywhere, the radius of convergence is infinite. √ 2/2 = 9. The sine of π/4 radians (45◦ ) is 0.70710678 . . .. How many terms in the series sin (x) = x − x5 x7 x3 + − + ··· 3! 5! 7! must be taken to achieve 1% accuracy at x = π/4? π = 0.785398 4 x3 x− = 0.785398 − 0.080746 = 0.704653 3! CHAPTER | 10 Mathematical Series e61 This is accurate to about 0.4%, so only two terms are needed. 11. Estimate the largest value of x that allows e x to be approximated to 1% accuracy by the following partial sum e x ≈ 1 + x. The function is not analytic at x = 0, so the interval of convergence is 0 ≺ x ≺ 2 • 0.20000 1.20000 1.221402758 1.78 • 0.19000 1.19000 1.209249598 1.62 • 0.18000 1.18000 1.197217363 1.46 • 0.17000 1.17000 1.185304851 1.31 1 = b0 + b1 (x − 2) + b2 (x − 2)2 + · · · x 1 1 b0 = = 2 2 1 1 b1 = − 2 = − x 2 4 1 2 1 = b2 = 2! x 3 2 8 1 6 1 =− b3 = − 2! x 4 2 16 • 0.15000 1.15000 1.161834243 1.03 The coefficients follow a regular pattern so that • 0.14000 1.14000 1.150273799 0.90 • 0.14500 1.14500 1.156039570 0.96 • 0.14777 1.14777 1.159246239 0.9999 Here is a table of values: ' a. • x difference 1 + x $ ex % bn = ( − 1)n • By trial and error, 1% accuracy is obtained with x ≺ 0.14777. & % 13. Find two different Taylor series to represent the function 1 f (x) = x such that one series is f (x) = a0 + a1 (x − 1) + a2 (x − 1)2 + · · · and the other is 2 f (x) = b0 + b1 (x − 2) + b3 (x − 2) + · · · Show that bn = an /2n for any value of n. Find the interval of convergence for each series (the ratio test may be used). Which series must you use in the vicinity of x = 3? Why? Find the Taylor series in powers of (x − 10) that represents the function ln (x). 1 = a0 + a1 (x − 1) + a2 (x − 1)2 + · · · x 1 a0 = = 1 1 1 a1 = − 2 = −1 x 1 1 2 a2 = =1 2! x 3 1 1 6 a3 = − =1 2! x 4 1 The coefficients follow a regular pattern so that 1 = 1 − (x − 1) + (x − 1)2 an = ( − 1) x −(x − 1)3 + (x − 1)4 + · · · n 1 an = n 2n 2 1 1 1 1 = − (x − 1) + (x − 1)2 x 2 4 8 1 1 3 − (x − 1) + (x − 1)4 + · · · 16 32 The function is not analytic at x = 0, so the interval of convergence is 0 ≺ x ≺ 4. The second series must be used for x = 3, since this value of x is outside the region of convergence of the first series. 15. Using the Maclaurin series for e x , show that the derivative of e x is equal to e x . x3 x4 x2 + + + ··· 2! 3! 4! d x 3x 2 4x 3 2x e = 0+1+ + + + ··· dx 2! 3! 4! x2 x3 = 1+x + + + · · · = ex 2! 3! ex = 1 + x + 17. Find the Taylor series for sin (x), expanding around π/2. sin (x) = a0 + a1 (x − π/2) + a2 (x − π/2)2 +a3 (x − π/2)3 + · · · a0 = sin π/2 = 1 1 dn an = sin (x) n n! d x π/2 df = cos (x) dx a1 = cos π/2 = 0 d2 f = − sin (x) dx 2 1 1 a2 = − sin π/2 = − 2! 2! e62 Mathematics for Physical Chemistry d3 f = − cos (x) dx 3 1 a3 = − cos π/2 = 0 3! d4 f = sin (x) dx 4 1 1 sin (π/2) = a4 = 4! 4! There is a pattern. Only even values of n occur,and signs alternate. 1 1 sin (x) = 1 − (x − π/2)2 + (x − π/2)4 2! 4! 1 − (x − π/2)6 + · · · 6! 19. Find the interval of convergence for the series for cos (x). cos (x) = 1 − x4 x6 x2 + − + ··· 2! 4! 6! Apply the alternating series test. Each term is smaller than the previous term if x is finite and if you go far enough into the series. The series converges for all finite values of x. 21. Using the Maclaurin series, show that x1 x es dx = e x 01 = e x1 − 1 0 x 0 x x2 x3 x4 1+x + + + + · · · dx 2! 3! 4! 0 x1 2 3 4 x x x + + + · · · = x+ 2 (3)2! (4)3! 0 es dx = x3 x4 x2 + + + ··· − 1 = 1+x + 2! 3! 4! x1 = e −1 23. Find the first few terms of the two-variable Maclaurin series representing the function f (x,y) = sin (x + y) f (0,0) ∂ f ∂x y 0,0 ∂ f ∂ y x 0,0 2 ∂ f ∂ y∂ x 0,0 2 ∂ f ∂ x 2 0,0 2 ∂ f ∂ y 2 0,0 3 ∂ f ∂ y∂ x 2 0,0 3 ∂ f ∂ y 2 ∂ x 0,0 4 ∂ f ∂ y 2 ∂ x 2 0,0 ∂5 f ∂ y2∂ x 3 = sin (0) = 0 = cos (x + y)|0,0 = 1 = cos (x + y)|0,0 = 1 = − sin (x + y)|0,0 = 1 = − sin (x + y)|0,0 = 0 = − sin (x + y)|0,0 = 0 = − cos (x + y) 0,0 = −1 = − cos (x + y) 0,0 = −1 = sin (x + y) 0,0 = 0 = cos (x + y) 0,0 = 1 0,0 There is a pattern. If n + m is even, the derivative vanishes. If n + m is odd, the derivative has magnitude 1 with alternating signs. 1 (x 2 y + x y 2 ) sin (x + y) = x + y − 1!2! 1 1 (x 2 y 3 + x 3 y 2 ) − (x 4 y 3 + x 3 y 4 ) + · · · + 3!2! 3!4!