Answer on Querstion #49111 - Math - Complex Analysis:
Find an integral ∫ 0 2 π e e i θ d θ \int_0^{2\pi}e^{e^{i\theta}}d\theta ∫ 0 2 π e e i θ d θ .
Solution
We can't use all of the standard tricks and tools of integration like substitution, trig substitution, parts. I think the best choice is to use Taylor formula. Let's denote e θ = t e^{\theta} = t e θ = t and we will have the next e t e^t e t .
Now we will use Taylor series and we will have the next expression:
1 + t 1 ! + t 2 2 ! + t 3 3 ! + … 1 + \frac {t}{1 !} + \frac {t ^ {2}}{2 !} + \frac {t ^ {3}}{3 !} + \dots 1 + 1 ! t + 2 ! t 2 + 3 ! t 3 + …
Now let's integrate our expression and we will have the next:
∫ 0 2 π e e i θ d θ = ∫ 0 2 π ( 1 + e i θ 1 ! + e 2 i θ 2 ! + e 3 i θ 3 ! + … ) d θ = 1 ∣ 0 2 π = 2 π \int_ {0} ^ {2 \pi} e ^ {e ^ {i \theta}} d \theta = \int_ {0} ^ {2 \pi} \left(1 + \frac {e ^ {i \theta}}{1 !} + \frac {e ^ {2 i \theta}}{2 !} + \frac {e ^ {3 i \theta}}{3 !} + \dots\right) d \theta = 1 \Big | _ {0} ^ {2 \pi} = 2 \pi ∫ 0 2 π e e i θ d θ = ∫ 0 2 π ( 1 + 1 ! e i θ + 2 ! e 2 i θ + 3 ! e 3 i θ + … ) d θ = 1 ∣ ∣ 0 2 π = 2 π
Here we will count integral with power n = 2 k + 1 n = 2k + 1 n = 2 k + 1 but we will show it for k = 0 k = 0 k = 0
∫ 0 2 π e i θ 1 ! d θ = 1 1 ! ( ∫ 0 2 π cos θ d θ + i ∫ 0 2 π sin θ d θ ) = 1 1 ! ( sin θ ∣ 0 2 π − cos θ ∣ 0 2 π ) = = 1 1 ! ( sin 2 π − sin 0 − i ( cos 2 π − cos 0 ) ) = 0 \begin{array}{l} \int_ {0} ^ {2 \pi} \frac {e ^ {i \theta}}{1 !} d \theta = \frac {1}{1 !} \left(\int_ {0} ^ {2 \pi} \cos \theta d \theta + i \int_ {0} ^ {2 \pi} \sin \theta d \theta\right) = \frac {1}{1 !} \left(\sin \theta \Big | _ {0} ^ {2 \pi} - \cos \theta \Big | _ {0} ^ {2 \pi}\right) = \\ = \frac {1}{1 !} (\sin 2 \pi - \sin 0 - i (\cos 2 \pi - \cos 0)) = 0 \\ \end{array} ∫ 0 2 π 1 ! e i θ d θ = 1 ! 1 ( ∫ 0 2 π cos θ d θ + i ∫ 0 2 π sin θ d θ ) = 1 ! 1 ( sin θ ∣ ∣ 0 2 π − cos θ ∣ ∣ 0 2 π ) = = 1 ! 1 ( sin 2 π − sin 0 − i ( cos 2 π − cos 0 )) = 0
Here we will count integral with power n = 2 k n = 2k n = 2 k but we will show it for k = 1 k = 1 k = 1
∫ 0 2 π e 2 i θ 2 ! d θ = 1 2 ! ( ∫ 0 2 π cos 2 θ d θ + i ∫ 0 2 π sin 2 θ d θ ) = 1 2 ! 1 2 ( sin 2 θ ∣ 0 2 π − cos 2 θ ∣ 0 2 π ) = = 1 2 ! 1 2 ( sin 4 π − sin 0 − i ( cos 4 π − cos 0 ) ) = 0 \begin{array}{l} \int_ {0} ^ {2 \pi} \frac {e ^ {2 i \theta}}{2 !} d \theta = \frac {1}{2 !} \left(\int_ {0} ^ {2 \pi} \cos 2 \theta d \theta + i \int_ {0} ^ {2 \pi} \sin 2 \theta d \theta\right) = \frac {1}{2 !} \frac {1}{2} \left(\sin 2 \theta \Big | _ {0} ^ {2 \pi} - \cos 2 \theta \Big | _ {0} ^ {2 \pi}\right) = \\ = \frac {1}{2 !} \frac {1}{2} (\sin 4 \pi - \sin 0 - i (\cos 4 \pi - \cos 0)) = 0 \\ \end{array} ∫ 0 2 π 2 ! e 2 i θ d θ = 2 ! 1 ( ∫ 0 2 π cos 2 θ d θ + i ∫ 0 2 π sin 2 θ d θ ) = 2 ! 1 2 1 ( sin 2 θ ∣ ∣ 0 2 π − cos 2 θ ∣ ∣ 0 2 π ) = = 2 ! 1 2 1 ( sin 4 π − sin 0 − i ( cos 4 π − cos 0 )) = 0
So we don't have any expressions with factorials.
And our integral will be next ∫ 0 2 π e e i θ d θ = 2 π \int_0^{2\pi}e^{e^{i\theta}}d\theta = 2\pi ∫ 0 2 π e e i θ d θ = 2 π
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