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1
1
1
1
x
a 1
x
a 2
x
a 3
x
a n
P
(
x
)=
...
Euler assumed that this property extends to “infinite polynomials” and applied it to
sin x
/
x . Namely, sin x
/
x is equal to zero in correspondence to the following values
of x :
π ,− π ,
2
π ,−
2
π ,
3
π ,−
3
π ...
whence:
1
1
1
1
x 2
3! +
x 4
5!
x 6
7! +
x 8
9! ... =
x
π
x
π
x
2
x
...
1
π
2
π
that is:
1
1
1
x 2
3! +
x 4
5!
x 6
7! +
x 8
9! ... =
x 2
π
x 2
4
x 2
9
1
...
2
2
2
π
π
or equivalently:
1
π
x 2
x 2
3! +
x 4
5!
x 6
7! +
x 8
9! ... =
1
1
1
1
2 +
2 +
2 + ...
...
4
π
9
π
therefore, by equating the coefficients of x 2
of the two members (the other powers
do not matter, in this context), we get:
1
1
3! =
1
π
1
4 +
1
9 +
1
16 + ...
+
2
thereby concluding that:
2
6 .
1
4 +
1
9 +
16 + ... = π
1
1
+
The sin x
x representation, in terms of its infinite roots, provides another important
result due to Wallis, which we use to prove Stirling's approximation (see Sect. 7.5).
In fact:
/
1
1
1
1
2
2 2
2
2 2
2
2 2
2
2 2
sin
( π /
2
)
π
/
π
/
π
/
π
/
2 =
...
2
2
2
2
π /
π
4
π
9
π
16
π
that is:
π = (
2
4
1
)
(
16
1
)
(
36
1
)
...
4
16
36
which is exactly Wallis' identity, usually given by the following equality:
2
π =
1
·
3
·
3
·
5
·
5
·
7
·
7
·
9
...
... .
2
·
2
·
4
·
4
·
6
·
6
·
8
·
8
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