For all x∈R, let
f(x)=∫π0sin(t)1+cos2(xt)dt
Compute the limit when x→+∞.
My attempt :
I tried the substitution u=sin(t) (and u=cos2(xt)) but it seems worse:
∫10u(1+(cos(xarcsin(u)))2)√1−u2du
I tried to use a subsequence (xn) which is tends to +∞ and use the dominated convergence theorem but it didn't work either.
Sorry if my attempt doesn't make much sense.
Thank you in advance.
Answer
We can use a generalization of the Riemann-Lebesgue lemma that states that if f(x) is a continuous function on [a,b], where 0≤a<b, and g(x) is a continuous T-periodic function on [0,∞), then lim
A proof can be found in THIS PAPER.
The proof uses the fact that a primitive of g(x) can be expressed as \int_{0}^{x} g(t) \, dt = \frac{x}{T} \int_{0}^{T} g(t) \ dt + h(x), where h(x) is T-periodic function. (Lemma 2.2)
The regular Riemann-Lesbegue lemma is the case where the average value of g(x) is 0.
Applying the lemma to this particular integral, we get
\lim_{x \to \infty} \int_{0}^{\pi} \frac{\sin t}{1+\cos^{2}(xt)} \ dt = \left( \frac{1}{\pi} \int_{0}^{\pi} \frac{1}{1+\cos^{2} t} \ dt \right) \left( \int_{0}^{\pi} \sin t \ dt \right).
The first integral can be evaluated by making the substitution u = \tan t.
This particular example actually appears in the paper, so I'll omit the details.
We end up with
\lim_{x \to \infty} \int_{0}^{\pi} \frac{\sin t}{1+\cos^{2}(xt)} \ dt = \frac{1}{\pi} \left(\frac{\pi}{\sqrt{2}} \right) \left(2\right) = \sqrt{2} .
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