In the 1760s, Johann Heinrich Lambert was the first to prove that the number is irrational, meaning it cannot be expressed as a fraction
a/b
a
b
In 1882, Ferdinand von Lindemann proved that
\pi
In 1761, Johann Heinrich Lambert proved that
\pi
\tan(x)=\cfrac{x}{1-\cfrac{x2}{3-\cfrac{x2}{5-\cfrac{x2}{7-{}\ddots}}}}.
Then Lambert proved that if
x
\tan\tfrac\pi4=1
\tfrac\pi4
\pi
Written in 1873, this proof uses the characterization of
\pi
\pi2
Consider the sequences of real functions
An
Un
n\in\N0
\begin{align} A0(x)&=\sin(x),&&An+1(x)
xyA | |
=\int | |
n(y)dy |
\\[4pt] U0(x)&=
\sin(x) | |
x, |
&&Un+1(x)=-
Un'(x) | |
x \end{align} |
Using induction we can prove that
\begin{align} An(x)&=
x2n+1 | - | |
(2n+1)!! |
x2n+3 | + | |
2 x (2n+3)!! |
x2n+5 | |
2 x 4 x (2n+5)!! |
\mp … \\[4pt] Un(x)&=
| ||||
|
\mp … \end{align}
and therefore we have:
U | ||||
|
.
So
\begin{align} | An+1(x) |
x2n+3 |
&=Un+1(x)=-
Un'(x) | |||||||||
|
\right)\\[6pt] &=-
1 | |
x |
\left(
An'(x) ⋅ x2n+1-(2n+1)x2nAn(x) | |
x2(2n+1) |
\right)\\[6pt] &=
(2n+1)An(x)-xAn'(x) | |
x2n+3 |
\end{align}
which is equivalent to
An+1
2A | |
(x)=(2n+1)A | |
n-1 |
(x).
Using the definition of the sequence and employing induction we can show that
An(x)=
2) | |
P | |
n(x |
\sin(x)+x
2) | |
Q | |
n(x |
\cos(x),
where
Pn
Qn
Pn
l\lfloor\tfrac12nr\rfloor.
Anl(\tfrac12\pir)=
2r). | |
P | |
nl(\tfrac14\pi |
Hermite also gave a closed expression for the function
An,
A | ||||
|
1(1-z | |
\int | |
0 |
2)n\cos(xz)dz.
He did not justify this assertion, but it can be proved easily. First of all, this assertion is equivalent to
1 | |
2nn! |
1(1-z | |
\int | |
0 |
2)n\cos(xz)dz=
An(x) | |
x2n+1 |
=Un(x).
Proceeding by induction, take
n=0.
| ||||
\int | ||||
0(x) |
n.
1 | |
2nn! |
1(1-z | |
\int | |
0 |
2)
n\cos(xz)dz=U | |
n(x), |
then, using integration by parts and Leibniz's rule, one gets
\begin{align} & | 1 |
2n+1(n+1)! |
1\left(1-z | |
\int | |
0 |
2\right)n+1\cos(xz)dz\\ & =
1 | |
2n+1(n+1)! |
l(\overbrace{\left.(1-z2)n+1
\sin(xz) | |
x\right| |
z=1 | |
z=0 |
If
\tfrac14\pi2=p/q,
p
q
\N
Pn
l\lfloor\tfrac12nr\rfloor,
q\lfloor
2r) | |
P | |
nl(\tfrac14\pi |
N.
N=q\lfloor{An}l(\tfrac12\pir)=q\lfloor
1 | |
2nn! |
\left(\dfracpq
| ||||
\right) |
1(1-z | |
\int | |
0 |
2)n\cos\left(\tfrac12\piz\right)dz.
But this number is clearly greater than
0.
n
n
N<1.
Hermite did not present his proof as an end in itself but as an afterthought within his search for a proof of the transcendence of
\pi.
e
Moreover, Hermite's proof is closer to Lambert's proof than it seems. In fact,
An(x)
\tanx.
Harold Jeffreys wrote that this proof was set as an example in an exam at Cambridge University in 1945 by Mary Cartwright, but that she had not traced its origin. It still remains on the 4th problem sheet today for the Analysis IA course at Cambridge University.[7]
Consider the integrals
In(x)=\int
1(1 | |
-1 |
-z2)n\cos(xz)dz,
where
n
Two integrations by parts give the recurrence relation
2I | |
x | |
n(x)=2n(2n-1)I |
n-1(x)-4n(n-1)In-2(x). (n\geq2)
If
2n+1 | |
J | |
n(x)=x |
In(x),
then this becomes
Jn(x)=2n(2n-1)Jn-1
2J | |
(x)-4n(n-1)x | |
n-2 |
(x).
Furthermore,
J0(x)=2\sinx
J1(x)=-4x\cosx+4\sinx.
n\in\Z+,
2n+1 | |
J | |
n(x)=x |
In(x)=n!l(Pn(x)\sin(x)+Qn(x)\cos(x)r),
where
Pn(x)
Qn(x)
\leqn,
Take
x=\tfrac12\pi,
\tfrac12\pi=a/b
a
b
\pi
a2n+1 | |
n! |
Inl(\tfrac12\pir)=
2n+1 | |
P | |
nl(\tfrac12\pir)b |
.
The right side is an integer. But
0<Inl(\tfrac12\pir)<2
[-1,1]
2
0
1.
a2n+1 | |
n! |
\to0 asn\toinfty.
Hence, for sufficiently large
n
0<
| ||||||||||||||
n! |
<1,
that is, we could find an integer between
0
1.
\pi
This proof is similar to Hermite's proof. Indeed,
2n+1 | |
\begin{align} J | |
n(x)&=x |
1 | |
\int | |
-1 |
(1-z2)n\cos(xz)dz\\[5pt] &=2x2n+1
1 | |
\int | |
0 |
(1-z2)n\cos(xz)dz\\[5pt] &=2n+1n!An(x). \end{align}
However, it is clearly simpler. This is achieved by omitting the inductive definition of the functions
An
This proof uses the characterization of
\pi
Suppose that
\pi
\pi=a/b
a
b
n,
f(x)=
xn(a-bx)n | |
n! |
and, for each
x\in\R
F(x)=f(x)-f''(x)+f(4)(x)+ … +(-1)nf(2n)(x).
Claim 1:
F(0)+F(\pi)
Proof:Expanding
f
xk
ck/n!
ck
0
k<n.
f(k)(0)
0
k<n
(k!/n!)ck
f(k)(0)
F(0)
On the other hand,
f(\pi-x)=f(x)
(-1)kf(k)(\pi-x)=f(k)(x)
k.
(-1)kf(k)(\pi)=f(k)(0).
f(k)(\pi)
F(\pi)
F(0)
F(\pi)
Claim 2:
\pi | |
\int | |
0 |
f(x)\sin(x)dx=F(0)+F(\pi)
Proof: Since
f(2n
F''+F=f.
The derivatives of the sine and cosine function are given by sin' = cos and cos' = -sin. Hence the product rule implies
(F' ⋅ \sin{}-F ⋅ \cos{})'=f ⋅ \sin
By the fundamental theorem of calculus
\left.
\pi | |
\int | |
0 |
f(x)\sin(x)dx=l(F'(x)\sinx-F(x)\cosxr)
\pi. | |
\right| | |
0 |
Since
\sin0=\sin\pi=0
\cos0=-\cos\pi=1
\pi
Conclusion: Since
f(x)>0
\sinx>0
0<x<\pi
\pi
F(0)+F(\pi)
0\leqx(a-bx)\leq\pia
0\leq\sinx\leq1
0\leqx\leq\pi,
f,
\pi | ||
\int | f(x)\sin(x)dx\le\pi | |
0 |
(\pia)n | |
n! |
which is smaller than
1
n,
F(0)+F(\pi)<1
n,
F(0)+F(\pi).
\pi
The above proof is a polished version, which is kept as simple as possible concerning the prerequisites, of an analysis of the formula
\pi | |
\int | |
0 |
f(x)\sin(x)dx=
n | |
\sum | |
j=0 |
(-1)j\left(f(2j)(\pi)+f(2j)(0)\right)+(-1)n+1
\pi | |
\int | |
0 |
f(2n+2)(x)\sin(x)dx,
which is obtained by
2n+2
F
f(2n+2)
Niven's proof is closer to Cartwright's (and therefore Hermite's) proof than it appears at first sight.[6] In fact,
2n+1 | |
\begin{align} J | |
n(x)&=x |
1(1-z | |
\int | |
-1 |
2)
1\left | |
-1 |
(x2-(xz)2\right)nx\cos(xz)dz. \end{align}
xz=y
x(x | |
\int | |
-x |
2-y2)n\cos(y)dy.
In particular,
\pi/2 | |||||
\begin{align} J | \left( | ||||
|
\pi2 | |
4-y |
2\right)
| |||||||
0 |
| ||||
\piyn(\pi-y)
| ||||
\pi | |
\int | |
0 |
f(x)\sin(x)dx. \end{align}
Another connection between the proofs lies in the fact that Hermite already mentions[3] that if
f
F=f-f(2)+f(4)\mp … ,
then
\intf(x)\sin(x)dx=F'(x)\sin(x)-F(x)\cos(x)+C,
from which it follows that
\pi | |
\int | |
0 |
f(x)\sin(x)dx=F(\pi)+F(0).
Bourbaki's proof is outlined as an exercise in his calculus treatise. For each natural number b and each non-negative integer
n,
| ||||
A | ||||
0 |
\sin(x)dx.
Since
An(b)
[0,\pi]
0
0
\pi
0
An(b)>0.
b,
An(b)<1
n
x(\pi-x)\le\left(
\pi2\right) | |
2 |
and therefore
An(b)\le\pibn
1 | \left( | |
n! |
\pi2\right) | |
2n |
=\pi
(b\pi2/4)n | |
n! |
.
On the other hand, repeated integration by parts allows us to deduce that, if
a
b
\pi=a/b
f
[0,\pi]
\R
f(x)= | xn(a-bx)n |
n! |
,
then:
\begin{align} An(b)&=
\pi | |
\int | |
0 |
f(x)\sin(x)dx\\[5pt] &=
x=\pi | |
[{-f(x)\cos(x)}] | |
x=0 |
-[{-f'(x)\sin(x)}
x=\pi | |
] | |
x=0 |
+ … \\[5pt] & \pm[f(2n)(x)\cos(x)
x=\pi | |
] | |
x=0 |
\pm
\pi | |
\int | |
0 |
f(2n+1)(x)\cos(x)dx. \end{align}
This last integral is
0,
f(2n+1)
f
f(k)
0
\pi
An(b)
0,
An(b)<1
n
This proof is quite close to Niven's proof, the main difference between them being the way of proving that the numbers
An(b)
Miklós Laczkovich's proof is a simplification of Lambert's original proof. He considers the functions
fk(x)=1-
x2 | - | ||
|
x6 | |
3!k(k+1)(k+2) |
+ … (k\notin\{0,-1,-2,\ldots\}).
These functions are clearly defined for any real number
x.
f1/2(x)=\cos(2x),
f3/2(x)=
\sin(2x) | |
2x |
.
Claim 1: The following recurrence relation holds for any real number
x2 | |
k(k+1) |
fk+2(x)=fk+1(x)-fk(x).
Proof: This can be proved by comparing the coefficients of the powers of
x.
Claim 2: For each real number
x,
\limk\to+inftyfk(x)=1.
Proof: In fact, the sequence
x2n/n!
C
k>1,
\left|fk(x)-1\right|\leqslant\sum
| ||||||||||||
= | ||||||||||||
n=1 |
C{k-1}. | |
Claim 3: If
x ≠ 0,
x2
k\in\Q\smallsetminus\{0,-1,-2,\ldots\}
fk(x) ≠ 0 and
fk+1(x) | |
fk(x) |
\notin\Q.
Proof: Otherwise, there would be a number
y ≠ 0
a
b
fk(x)=ay
fk+1(x)=by.
y=fk+1(x),
a=0,
b=1
a
b
fk+1(x)/fk(x)=b/a
y=fk(x)/a=fk+1(x)/b.
y
0,
fk+n(x)
n\in\N
0,
c
bc/k,
ck/x2,
c/x2
gn=\begin{cases}fk(x)&
n}{k(k+1) … (k+n-1)}f | |
n=0\ \dfrac{c | |
k+n |
(x)&n ≠ 0\end{cases}
Then
g0=fk(x)=ay\in\Zy and
g | (x)= | ||||
|
bc | |
ky\in\Z |
y.
On the other hand, it follows from claim 1 that
\begin{align} gn+2&=
cn+2 | ⋅ | |
x2k(k+1) … (k+n-1) |
x2 | |
(k+n)(k+n+1) |
fk+n+2(x)\\[5pt] &=
cn+2 | |
x2k(k+1) … (k+n-1) |
fk+n+1(x)-
cn+2 | |
x2k(k+1) … (k+n-1) |
fk+n(x)\\[5pt] &=
c(k+n) | |
x2 |
gn+1-
c2 | |
x2 |
g | + | ||||
|
c{x | |
2}n\right)g |
n+1-
c2 | |
x2 |
gn, \end{align}
which is a linear combination of
gn+1
gn
gn
y.
gn
0
n
gn
0.
|y|
0.
Since
f1/2(\tfrac14\pi)=\cos\tfrac12\pi=0,
\tfrac1{16}\pi2
\pi
On the other hand, since
\tanx=
\sinx | =x | |
\cosx |
f3/2(x/2) | |
f1/2(x/2) |
,
another consequence of Claim 3 is that, if
x\in\Q\smallsetminus\{0\},
\tanx
Laczkovich's proof is really about the hypergeometric function. In fact,
fk(x)={}0F1(k-x2)
Laczkovich's result can also be expressed in Bessel functions of the first kind
J\nu(x)
\Gamma(k)Jk-1(2x)=xk-1fk(x)
\Gamma
x ≠ 0,
x2
k\in\Q\smallsetminus\{0,-1,-2,\ldots\}
xJk(x) | |
Jk-1(x) |
\notin\Q.