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We'll evaluate ∫ 0 ∞ x 2 + 1 cos ( 3 x ) d x using complex integration.
First, we'll evaluate the related integral ∫ C 1 + z 2 e 3 i z d z where C is the loop in the complex pane consisting of the real interval [ − R , R ] and the semicircle γ lying above [ − R , R ] , for some large real number R .
We have ∫ C 1 + z 2 e 3 i z d z = ∫ − R R 1 + x 2 e 3 i x d x + ∫ γ 1 + z 2 e 3 i z d z . ( ∗ )
Note 1 + z 2 e 3 i z = ( z − i ) ( z + i ) e 3 i z has two simple poles located at i , − i . Only i lies in the region enclosed by C . By Cauchy's integration formula, ∫ C 1 + z 2 e 3 i z d z = 2 π i ⋅ i + i e 3 i ⋅ i = e 3 π . ( ∗ ∗ )
We find an upper bound on the integral over γ by paramaterizing z = R e i t , t ∈ [ 0 , π ] :
∣ ∣ ∣ ∣ ∫ γ 1 + z 2 e 3 i z d z ∣ ∣ ∣ ∣ = ∣ ∣ ∣ ∣ ∫ 0 π 1 + R 2 e 2 i t e 3 i R e i t R i e i t d t ∣ ∣ ∣ ∣ ≤ ∫ 0 π ∣ ∣ ∣ ∣ 1 + R 2 e 2 i t e 3 i R e i t R i e i t ∣ ∣ ∣ ∣ d t
= ∫ 0 π R 2 − 1 ∣ R e 3 i R ( cos ( t ) + i sin ( t ) ) ∣ d t = ∫ 0 π R 2 − 1 R e − 3 R sin ( t )
≤ ∫ 0 π R 2 − 1 R d t = R 2 − 1 π R → 0 as R → ∞ .
Thus, as R → ∞ , the integral over γ goes to 0 . ( ∗ ∗ ∗ )
Then letting R → ∞ , we find from ( ∗ ) , ( ∗ ∗ ) , and ( ∗ ∗ ∗ ) :
e 3 π = ∫ − ∞ ∞ 1 + x 2 e 3 i x d x
ℜ ( e 3 π ) = ℜ ( ∫ − ∞ − ∞ 1 + x 2 e 3 i x d x )
e 3 π = ∫ − ∞ ∞ 1 + x 2 cos ( 3 x ) d x .
Then since 1 + x 2 cos ( 3 x ) is an even function, we are left with
∫ 0 ∞ 1 + x 2 cos ( 3 x ) d x = 2 1 ∫ − ∞ ∞ 1 + x 2 cos ( 3 x ) d x = 2 e 3 π .
We use a calculator to find 1 0 4 2 e 3 π ≈ 7 8 2 . 1 , so the answer is 7 8 2 .