Harmonic series (mathematics)
Divergent means that as you add more terms the sum never stops getting bigger. It does not go towards a single finite value.
Infinite means that you can always add another term. There is no final term to the series.
Its name comes from the idea of harmonics in music: the wavelengths of the overtones of a vibrating string are 1/, 1/, 1/, etc., of the string's fundamental wavelength. Apart from the first term, every term of the series is the harmonic mean of the terms either side of it. The phrase harmonic mean also comes from music.
The fact that the harmonic series diverges was first proven in the 14th century by Nicole Oresme, but was forgotten. Proofs were given in the 17th century by Pietro Mengoli, Johann Bernoulli, and Jacob Bernoulli.
Harmonic sequences have been used by architects. In the Baroque period architects used them in the proportions of floor plans, elevations, and in the relationships between architectural details of churches and palaces.
There are several well-known proofs of the divergence of the harmonic series. A few of them are given below.
One way to prove divergence is to compare the harmonic series with another divergent series, where each denominator is replaced with the next-largest power of two:
Each term of the harmonic series is greater than or equal to the corresponding term of the second series, and therefore the sum of the harmonic series must be greater than or equal to the sum of the second series. However, the sum of the second series is infinite:
It follows (by the comparison test) that the sum of the harmonic series must be infinite as well. More precisely, the comparison above proves that
It is possible to prove that the harmonic series diverges by comparing its sum with an improper integral. Consider the arrangement of rectangles shown in the figure to the right. Each rectangle is 1 unit wide and 1/ units high, so the total area of the infinite number of rectangles is the sum of the harmonic series:
The total area under the curve y = 1/ from 1 to infinity is given by a divergent improper integral:
Since this area is entirely contained within the rectangles, the total area of the rectangles must be infinite as well. This proves that
The generalization of this argument is known as the integral test.
Rate of divergenceEdit
where γ is the Euler–Mascheroni constant and εk ~ 1/ which approaches 0 as k goes to infinity. Leonhard Euler proved both this and also that the sum which includes only the reciprocals of primes also diverges, that is:
|n||Partial sum of the harmonic series, Hn|
|expressed as a fraction||decimal||relative size|
The finite partial sums of the diverging harmonic series,
are called harmonic numbers.
The difference between Hn and ln n converges to the Euler–Mascheroni constant. The difference between any two harmonic numbers is never an integer. No harmonic numbers are integers, except for H1 = 1.:p. 24:Thm. 1
Alternating harmonic seriesEdit
The alternating harmonic series, while conditionally convergent, is not absolutely convergent: if the terms in the series are systematically rearranged, in general the sum becomes different and, dependent on the rearrangement, possibly even infinite.
A related series can be derived from the Taylor series for the arctangent:
This is known as the Leibniz series.
General harmonic seriesEdit
The general harmonic series is of the form
where a ≠ 0 and b are real numbers, and b/ is not zero or a negative integer.
By the limit comparison test with the harmonic series, all general harmonic series also diverge.
A generalization of the harmonic series is the p-series (or hyperharmonic series), defined as
for any real number p. When p = 1, the p-series is the harmonic series, which diverges. Either the integral test or the Cauchy condensation test shows that the p-series converges for all p > 1 (in which case it is called the over-harmonic series) and diverges for all p ≤ 1. If p > 1 then the sum of the p-series is ζ(p), i.e., the Riemann zeta function evaluated at p.
The problem of finding the sum for p = 2 is called the Basel problem; Leonhard Euler showed it is π2/. The value of the sum for p = 3 is called Apéry's constant, since Roger Apéry proved that it is an irrational number.
Related to the p-series is the ln-series, defined as
for any positive real number p. This can be shown by the integral test to diverge for p ≤ 1 but converge for all p > 1.
For any convex, real-valued function φ such that
Random harmonic seriesEdit
The random harmonic series
where the sn are independent, identically distributed random variables taking the values +1 and −1 with equal probability 1/, is a well-known example in probability theory for a series of random variables that converges with probability 1. The fact of this convergence is an easy consequence of either the Kolmogorov three-series theorem or of the closely related Kolmogorov maximal inequality. Byron Schmuland of the University of Alberta further examined the properties of the random harmonic series, and showed that the convergent series is a random variable with some interesting properties. In particular, the probability density function of this random variable evaluated at +2 or at −2 takes on the value 0.124999999999999999999999999999999999999999764..., differing from 1/ by less than 10−42. Schmuland's paper explains why this probability is so close to, but not exactly, 1/. The exact value of this probability is given by the infinite cosine product integral C2 divided by π.
Depleted harmonic seriesEdit
The depleted harmonic series where all of the terms in which the digit 9 appears anywhere in the denominator are removed can be shown to converge and its value is less than 80. In fact, when all the terms containing any particular string of digits (in any base) are removed the series converges.
The harmonic series can be counterintuitive. This is because it is a divergent series even though the terms of the series get smaller and go towards zero. The divergence of the harmonic series is the source of some paradoxes.
- The "worm on the rubber band". Suppose that a worm crawls along an infinitely-elastic one-meter rubber band at the same time as the rubber band is uniformly stretched. If the worm travels 1 centimeter per minute and the band stretches 1 meter per minute, will the worm ever reach the end of the rubber band? The answer, counterintuitively, is "yes", for after n minutes, the ratio of the distance travelled by the worm to the total length of the rubber band is
Because the series gets arbitrarily large as n becomes larger, eventually this ratio must exceed 1, which implies that the worm reaches the end of the rubber band. However, the value of n at which this occurs must be extremely large: approximately e100, a number exceeding 1043 minutes (1037 years). Although the harmonic series does diverge, it does so very slowly.
- The Jeep problem asks how much total fuel is required for a car with a limited fuel-carrying capacity to cross a desert leaving fuel drops along the route. The distance the car can go with a given amount of fuel is related to the partial sums of the harmonic series, which grow logarithmically. And so the fuel required increases exponentially with the desired distance.
- The block-stacking problem: given a collection of identical dominoes, it is possible to stack them at the edge of a table so that they hang over the edge of the table without falling. The counterintuitive result is that they can be stacked in a way that makes the overhang as large as you want. That is, provided there are enough dominoes.
- A swimmer that goes faster each time they touch the wall of the pool. The swimmer starts crossing a 10-meter pool at a speed of 2 m/s, and with every crossing, another 2 m/s is added to the speed. In theory, the swimmer's speed is unlimited, but the number of pool crosses needed to get to that speed becomes very large; for instance, to get to the speed of light (ignoring special relativity), the swimmer needs to cross the pool 150 million times. Contrary to this large number, the time needed to reach a given speed depends on the sum of the series at any given number of pool crosses:
Calculating the sum shows that the time required to get to the speed of light is only 97 seconds.
- Oresme, Nicole (c. 1360). Quaestiones super Geometriam Euclidis [Questions concerning Euclid's Geometry].
- Mengoli, Pietro (1650). "Praefatio [Preface]". Novae quadraturae arithmeticae, seu De additione fractionum [New arithmetic quadrature (i.e., integration), or On the addition of fractions]. Bologna: Giacomo Monti.
Mengoli's proof is by contradiction:
- Let S denote the sum of the series. Group the terms of the series in triplets: S = 1 + (1/ + 1/ + 1/) + (1/ + 1/ + 1/) + (1/ + 1/ + 1/) + … Since for x > 1, 1/ + 1/ + 1/ > 3/, then S > 1 + 3/ + 3/ + 3/ + … = 1 + 1 + 1/ + 1/ + … = 1 + S, which is false for any finite S. Therefore, the series diverges.
- Bernoulli, Johann (1742). "Corollary III of De seriebus varia". Opera Omnia. Lausanne & Basel: Marc-Michel Bousquet & Co. vol. 4, p. 8.
- Bernoulli, Jacob (1689). Propositiones arithmeticae de seriebus infinitis earumque summa finita [Arithmetical propositions about infinite series and their finite sums]. Basel: J. Conrad.
- Bernoulli, Jacob (1713). Ars conjectandi, opus posthumum. Accedit Tractatus de seriebus infinitis [Theory of inference, posthumous work. With the Treatise on infinite series…]. Basel: Thurneysen. pp. 250–251.
From p. 250, prop. 16:
- "XVI. Summa serei infinita harmonicè progressionalium, 1/ + 1/ + 1/ + 1/ + 1/ &c. est infinita. Id primus deprehendit Frater:…"
- [16. The sum of an infinite series of harmonic progression, 1/ + 1/ + 1/ + 1/ + 1/ + …, is infinite. My brother first discovered this…]
- Hersey, George L. Architecture and Geometry in the Age of the Baroque. pp. 11–12, 37–51.
- Sloane, N. J. A. (ed.). "Sequence A082912 (Sum of a(n) terms of harmonic series is > 10n)". The On-Line Encyclopedia of Integer Sequences. OEIS Foundation.
- Julian Havil, Gamma: Exploring Euler’s Constant, Princeton University Press, 2009.
- Thomas J. Osler, “Partial sums of series that cannot be an integer”, The Mathematical Gazette 96, November 2012, 515–519. https://www.jstor.org/stable/24496876?seq=1#page_scan_tab_contents
- Schmuland, Byron (May 2003). "Random Harmonic Series" (PDF). American Mathematical Monthly. 110: 407–416. doi:10.2307/3647827.
- Eric W. Weisstein, Infinite Cosine Product Integral at MathWorld.
- "Nick's Mathematical Puzzles: Solution 72".
- Graham, Ronald; Knuth, Donald E.; Patashnik, Oren (1989), Concrete Mathematics (2nd ed.), Addison-Wesley, pp. 258–264, ISBN 978-0-201-55802-9
- Sharp, R. T. (1954). "Problem 52: Overhanging dominoes" (PDF). Pi Mu Epsilon Journal. 1 (10): 411–412.
|Wikimedia Commons has media related to Harmonic series.|
- "The Harmonic Series Diverges Again and Again" (PDF). The AMATYC Review. 27: 31–43. 2006.
- Eric W. Weisstein, Harmonic Series at MathWorld.
- Eric W. Weisstein, Book Stacking Problem at MathWorld.
- Hudelson, Matt (1 October 2010). "Proof Without Words: The Alternating Harmonic Series Sums to ln 2" (PDF). Mathematics Magazine. 83 (4): 294. doi:10.4169/002557010X521831.