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Proof that 22/7 exceedsπ

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This is not a perfect 22/7 circle, because 22/7 is not a perfect representation of pi.
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Proofs of the mathematical result that therational number22/7 is greater thanπ (pi) date back to antiquity. One of these proofs, more recently developed but requiring only elementary techniques from calculus, has attracted attention in modern mathematics due to itsmathematical elegance and its connections to the theory ofDiophantine approximations. Stephen Lucas calls this proof "one of the more beautiful results related to approximatingπ".[1]Julian Havil ends a discussion ofcontinued fraction approximations ofπ with the result, describing it as "impossible to resist mentioning" in that context.[2]

The purpose of the proof is not primarily to convince its readers that22/7(or⁠3+1/7) is indeed bigger than π. Systematic methods of computing the value ofπ exist. If one knows thatπ is approximately 3.14159, then it trivially follows thatπ < 22/7, which is approximately 3.142857. But it takes much less work to show thatπ < 22/7 by the method used in this proof than to show thatπ is approximately 3.14159.

Background

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22/7 is a widely usedDiophantine approximation ofπ. It is a convergent in the simplecontinued fraction expansion ofπ. It is greater thanπ, as can be readily seen in thedecimal expansions of these values:

227=3.142857¯,π=3.14159265{\displaystyle {\begin{aligned}{\frac {22}{7}}&=3.{\overline {142\,857}},\\\pi \,&=3.141\,592\,65\ldots \end{aligned}}}

The approximation has been known since antiquity.Archimedes wrote the first known proof that22/7 is an overestimate in the 3rd century BCE, although he may not have been the first to use that approximation. His proof proceeds by showing that22/7 is greater than the ratio of theperimeter of aregular polygon with 96 sides to the diameter of a circle it circumscribes.[note 1]

Proof

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The proof first devised by British electrical engineer Donald Percy Dalzell (1898–1988) in 1944[4] can be expressed very succinctly:

0<01x4(1x)41+x2dx=227π.{\displaystyle 0<\int _{0}^{1}{\frac {x^{4}\left(1-x\right)^{4}}{1+x^{2}}}\,dx={\frac {22}{7}}-\pi .}

Therefore,22/7 > π.

The evaluation of this integral was the first problem in the 1968Putnam Competition.[5]It is easier than most Putnam Competition problems, but the competition often features seemingly obscure problems that turn out to refer to something very familiar. This integral has also been used in the entrance examinations for theIndian Institutes of Technology.[6]

Details of evaluation of the integral

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That theintegral is positive follows from the fact that theintegrand isnon-negative; the denominator is positive and the numerator is a product of nonnegative numbers. One can also easily check that the integrand is strictly positive for at least one point in the range of integration, say at1/2. Since the integrand is continuous at that point and nonnegative elsewhere, the integral from 0 to 1 must be strictly positive.

It remains to show that the integral in fact evaluates to the desired quantity:

0<01x4(1x)41+x2dx=01x44x5+6x64x7+x81+x2dxexpansion of terms in the numerator=01(x64x5+5x44x2+441+x2)dx using polynomial long division=(x772x63+x54x33+4x4arctanx)|01definite integration=1723+143+4πwith arctan(1)=π4 and arctan(0)=0=227π.addition{\displaystyle {\begin{aligned}0&<\int _{0}^{1}{\frac {x^{4}\left(1-x\right)^{4}}{1+x^{2}}}\,dx\\[8pt]&=\int _{0}^{1}{\frac {x^{4}-4x^{5}+6x^{6}-4x^{7}+x^{8}}{1+x^{2}}}\,dx&{\text{expansion of terms in the numerator}}\\[8pt]&=\int _{0}^{1}\left(x^{6}-4x^{5}+5x^{4}-4x^{2}+4-{\frac {4}{1+x^{2}}}\right)\,dx&{\text{ using polynomial long division}}&\\[8pt]&=\left.\left({\frac {x^{7}}{7}}-{\frac {2x^{6}}{3}}+x^{5}-{\frac {4x^{3}}{3}}+4x-4\arctan {x}\right)\,\right|_{0}^{1}&{\text{definite integration}}\\[6pt]&={\frac {1}{7}}-{\frac {2}{3}}+1-{\frac {4}{3}}+4-\pi \quad &{\text{with }}\arctan(1)={\frac {\pi }{4}}{\text{ and }}\arctan(0)=0\\[8pt]&={\frac {22}{7}}-\pi .&{\text{addition}}\end{aligned}}}

(Seepolynomial long division.)

Quick upper and lower bounds

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InDalzell (1944), it is pointed out that if 1 is substituted forx in the denominator, one gets a lower bound on the integral, and if 0 is substituted forx in the denominator, one gets an upper bound:[7]

11260=01x4(1x)42dx<01x4(1x)41+x2dx<01x4(1x)41dx=1630.{\displaystyle {\frac {1}{1260}}=\int _{0}^{1}{\frac {x^{4}\left(1-x\right)^{4}}{2}}\,dx<\int _{0}^{1}{\frac {x^{4}\left(1-x\right)^{4}}{1+x^{2}}}\,dx<\int _{0}^{1}{\frac {x^{4}\left(1-x\right)^{4}}{1}}\,dx={1 \over 630}.}

Thus we have

2271630<π<22711260,{\displaystyle {\frac {22}{7}}-{\frac {1}{630}}<\pi <{\frac {22}{7}}-{\frac {1}{1260}},}

hence 3.1412 <π < 3.1421 in decimal expansion. The bounds deviate by less than 0.015% from π. See alsoDalzell (1971).[8]

Proof that 355/113 exceedsπ

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As discussed inLucas (2005), the well-known Diophantine approximation and far better upper estimate355/113 forπ follows from the relation

0<01x8(1x)8(25+816x2)3164(1+x2)dx=355113π.{\displaystyle 0<\int _{0}^{1}{\frac {x^{8}\left(1-x\right)^{8}\left(25+816x^{2}\right)}{3164\left(1+x^{2}\right)}}\,dx={\frac {355}{113}}-\pi .}
355113=3.14159292,{\displaystyle {\frac {355}{113}}=3.141\,592\,92\ldots ,}

where the first six digits after the decimal point agree with those ofπ. Substituting 1 forx in the denominator, we get the lower bound

01x8(1x)8(25+816x2)6328dx=9115261111856=0.000000173,{\displaystyle \int _{0}^{1}{\frac {x^{8}\left(1-x\right)^{8}\left(25+816x^{2}\right)}{6328}}\,dx={\frac {911}{5\,261\,111\,856}}=0.000\,000\,173\ldots ,}

substituting 0 forx in the denominator, we get twice this value as an upper bound, hence

3551139112630555928<π<3551139115261111856.{\displaystyle {\frac {355}{113}}-{\frac {911}{2\,630\,555\,928}}<\pi <{\frac {355}{113}}-{\frac {911}{5\,261\,111\,856}}\,.}

In decimal expansion, this means3.141592 57 <π <3.141592 74, where the bold digits of the lower and upper bound are those of π.

Extensions

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The above ideas can be generalized to get better approximations of π; see alsoBackhouse (1995)[9] andLucas (2005) (in both references, however, no calculations are given). For explicit calculations, consider, for every integern ≥ 1,

122n101x4n(1x)4ndx<122n201x4n(1x)4n1+x2dx<122n201x4n(1x)4ndx,{\displaystyle {\frac {1}{2^{2n-1}}}\int _{0}^{1}x^{4n}(1-x)^{4n}\,dx<{\frac {1}{2^{2n-2}}}\int _{0}^{1}{\frac {x^{4n}(1-x)^{4n}}{1+x^{2}}}\,dx<{\frac {1}{2^{2n-2}}}\int _{0}^{1}x^{4n}(1-x)^{4n}\,dx,}

where the middle integral evaluates to

122n201x4n(1x)4n1+x2dx=j=02n1(1)j22nj2(8nj1)(8nj24n+j)+(1)n(π4j=03n1(1)j2j+1){\displaystyle {\begin{aligned}{\frac {1}{2^{2n-2}}}&\int _{0}^{1}{\frac {x^{4n}(1-x)^{4n}}{1+x^{2}}}\,dx\\[6pt]={}&\sum _{j=0}^{2n-1}{\frac {(-1)^{j}}{2^{2n-j-2}(8n-j-1){\binom {8n-j-2}{4n+j}}}}+(-1)^{n}\left(\pi -4\sum _{j=0}^{3n-1}{\frac {(-1)^{j}}{2j+1}}\right)\end{aligned}}}

involving π. The last sum also appears inLeibniz' formula forπ. The correction term anderror bound is given by

122n101x4n(1x)4ndx=122n1(8n+1)(8n4n)πn210n2(8n+1),{\displaystyle {\begin{aligned}{\frac {1}{2^{2n-1}}}\int _{0}^{1}x^{4n}(1-x)^{4n}\,dx&={\frac {1}{2^{2n-1}(8n+1){\binom {8n}{4n}}}}\\[6pt]&\sim {\frac {\sqrt {\pi n}}{2^{10n-2}(8n+1)}},\end{aligned}}}

where the approximation (the tilde means that the quotient of both sides tends to one for largen) of thecentral binomial coefficient follows fromStirling's formula and shows the fast convergence of the integrals to π.

Calculation of these integrals: For all integersk ≥ 0 and ≥ 2 we have

xk(1x)=(12x+x2)xk(1x)2=(1+x2)xk(1x)22xk+1(1x)2.{\displaystyle {\begin{aligned}x^{k}(1-x)^{\ell }&=(1-2x+x^{2})x^{k}(1-x)^{\ell -2}\\[6pt]&=(1+x^{2})\,x^{k}(1-x)^{\ell -2}-2x^{k+1}(1-x)^{\ell -2}.\end{aligned}}}

Applying this formula recursively2n times yields

x4n(1x)4n=(1+x2)j=02n1(2)jx4n+j(1x)4n2(j+1)+(2)2nx6n.{\displaystyle x^{4n}(1-x)^{4n}=\left(1+x^{2}\right)\sum _{j=0}^{2n-1}(-2)^{j}x^{4n+j}(1-x)^{4n-2(j+1)}+(-2)^{2n}x^{6n}.}

Furthermore,

x6n(1)3n=j=13n(1)3njx2jj=03n1(1)3njx2j=j=03n1((1)3n(j+1)x2(j+1)(1)3njx2j)=(1+x2)j=03n1(1)3njx2j,{\displaystyle {\begin{aligned}x^{6n}-(-1)^{3n}&=\sum _{j=1}^{3n}(-1)^{3n-j}x^{2j}-\sum _{j=0}^{3n-1}(-1)^{3n-j}x^{2j}\\[6pt]&=\sum _{j=0}^{3n-1}\left((-1)^{3n-(j+1)}x^{2(j+1)}-(-1)^{3n-j}x^{2j}\right)\\[6pt]&=-(1+x^{2})\sum _{j=0}^{3n-1}(-1)^{3n-j}x^{2j},\end{aligned}}}

where the first equality holds, because the terms for1 ≤j ≤ 3n – 1 cancel, and the second equality arises from the index shiftjj + 1 in the first sum.

Application of these two results gives

x4n(1x)4n22n2(1+x2)=j=02n1(1)j22nj2x4n+j(1x)4n2j24j=03n1(1)3njx2j+(1)3n41+x2.(1){\displaystyle {\begin{aligned}{\frac {x^{4n}(1-x)^{4n}}{2^{2n-2}(1+x^{2})}}=\sum _{j=0}^{2n-1}&{\frac {(-1)^{j}}{2^{2n-j-2}}}x^{4n+j}(1-x)^{4n-2j-2}\\[6pt]&{}-4\sum _{j=0}^{3n-1}(-1)^{3n-j}x^{2j}+(-1)^{3n}{\frac {4}{1+x^{2}}}.\qquad (1)\end{aligned}}}

For integersk, ≥ 0, usingintegration by parts times, we obtain

01xk(1x)dx=k+101xk+1(1x)1dx=k+11k+21k+01xk+dx=1(k++1)(k+k).(2){\displaystyle {\begin{aligned}\int _{0}^{1}x^{k}(1-x)^{\ell }\,dx&={\frac {\ell }{k+1}}\int _{0}^{1}x^{k+1}(1-x)^{\ell -1}\,dx\\[6pt]&\,\,\,\vdots \\[6pt]&={\frac {\ell }{k+1}}{\frac {\ell -1}{k+2}}\cdots {\frac {1}{k+\ell }}\int _{0}^{1}x^{k+\ell }\,dx\\[6pt]&={\frac {1}{(k+\ell +1){\binom {k+\ell }{k}}}}.\qquad (2)\end{aligned}}}

Settingk = = 4n, we obtain

01x4n(1x)4ndx=1(8n+1)(8n4n).{\displaystyle \int _{0}^{1}x^{4n}(1-x)^{4n}\,dx={\frac {1}{(8n+1){\binom {8n}{4n}}}}.}

Integrating equation (1) from 0 to 1 using equation (2) andarctan(1) =π/4, we get the claimed equation involving π.

The results forn = 1 are given above. Forn = 2 we get

1401x8(1x)81+x2dx=π4717115015{\displaystyle {\frac {1}{4}}\int _{0}^{1}{\frac {x^{8}(1-x)^{8}}{1+x^{2}}}\,dx=\pi -{\frac {47\,171}{15\,015}}}

and

1801x8(1x)8dx=11750320,{\displaystyle {\frac {1}{8}}\int _{0}^{1}x^{8}(1-x)^{8}\,dx={\frac {1}{1\,750\,320}},}

hence3.141592 31 <π <3.141592 89, where the bold digits of the lower and upper bound are those of π. Similarly forn = 3,

11601x12(1x)121+x2dx=431302721137287920π{\displaystyle {\frac {1}{16}}\int _{0}^{1}{\frac {x^{12}\left(1-x\right)^{12}}{1+x^{2}}}\,dx={\frac {431\,302\,721}{137\,287\,920}}-\pi }

with correction term and error bound

13201x12(1x)12dx=12163324800,{\displaystyle {\frac {1}{32}}\int _{0}^{1}x^{12}(1-x)^{12}\,dx={\frac {1}{2\,163\,324\,800}},}

hence3.141592653 40 <π <3.141592653 87. The next step forn = 4 is

16401x16(1x)161+x2dx=π741269838109235953517800{\displaystyle {\frac {1}{64}}\int _{0}^{1}{\frac {x^{16}(1-x)^{16}}{1+x^{2}}}\,dx=\pi -{\frac {741\,269\,838\,109}{235\,953\,517\,800}}}

with

112801x16(1x)16dx=12538963567360,{\displaystyle {\frac {1}{128}}\int _{0}^{1}x^{16}(1-x)^{16}\,dx={\frac {1}{2\,538\,963\,567\,360}},}

which gives3.141592653589 55 <π <3.141592653589 96.

See also

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Footnotes

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Notes

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  1. ^Proposition 3: The ratio of the circumference of any circle to its diameter is less than⁠3+1/7 but greater than⁠3+10/71.[3]

Citations

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  1. ^Lucas, Stephen (2005),"Integral proofs that 355/113 > π"(PDF),Australian Mathematical Society Gazette,32 (4):263–266,MR 2176249,Zbl 1181.11077
  2. ^Havil, Julian (2003),Gamma. Exploring Euler's Constant, Princeton, NJ: Princeton University Press, p. 96,ISBN 0-691-09983-9,MR 1968276,Zbl 1023.11001
  3. ^Archimedes (2002) [1897], "Measurement of a circle", inHeath, T.L. (ed.),The Works of Archimedes, Dover Publications, pp. 93–96,ISBN 0-486-42084-1
  4. ^Nahin, Paul J. (2020).Inside Interesting Integrals. Springer Nature. p. 25.ISBN 978-3-030-43788-6.
  5. ^Alexanderson, Gerald L.; Klosinski, Leonard F.; Larson, Loren C., eds. (1985),The William Lowell Putnam Mathematical Competition: Problems and Solutions: 1965–1984, Washington, DC: The Mathematical Association of America,ISBN 0-88385-463-5,Zbl 0584.00003
  6. ^2010 IIT Joint Entrance Exam, question 41 on page 12 of the mathematics section.
  7. ^Dalzell, D. P. (1944), "On 22/7",Journal of the London Mathematical Society,19 (75 Part 3):133–134,doi:10.1112/jlms/19.75_part_3.133,MR 0013425,Zbl 0060.15306.
  8. ^Dalzell, D. P. (1971), "On 22/7 and 355/113",Eureka; the Archimedeans' Journal,34:10–13,ISSN 0071-2248.
  9. ^Backhouse, Nigel (July 1995), "Note 79.36, Pancake functions and approximations toπ",The Mathematical Gazette,79 (485):371–374,doi:10.2307/3618318,JSTOR 3618318,S2CID 126397479

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