Problem 33
Question
$$\begin{aligned} &\int_{0}^{\pi} \frac{d \theta}{(a+\cos \theta)^{2}}=\frac{1}{2} \int_{0}^{2 \pi} \frac{d \theta}{(a+\cos \theta)^{2}}=\frac{2}{i} \oint_{C} \frac{z}{\left(z^{2}+2 a z+1\right)^{2}} d z \quad(C \text { is }|z|=1)=\frac{2}{i} \oint_{C} \frac{z}{\left(z-r_{1}\right)^{2}\left(z-r_{2}\right)^{2}} d z\\\ &\text { where } r_{1}=-a+\sqrt{a^{2}-1}, r_{2}=-a-\sqrt{a^{2}-1} . \text { Now }\\\ &\oint_{C} \frac{z}{\left(z-r_{1}\right)^{2}\left(z-r_{2}\right)^{2}} d z=2 \pi i \operatorname{Res}\left(f(z), r_{1}\right)=2 \pi i \frac{a}{4(\sqrt{a^{2}-1})^{3}}=\frac{a \pi}{2(\sqrt{a^{2}-1})^{3}} i \end{aligned}$$ Thus $$\int_{0}^{\pi} \frac{d \theta}{(a+\cos \theta)^{2}}=\frac{2}{i} \cdot \frac{a \pi}{2(\sqrt{a^{2}-1})^{3}} i=\frac{a \pi}{(\sqrt{a^{2}-1})^{3}}$$ When \(a=2\) we obtain $$\begin{aligned} &\int_{0}^{\pi} \frac{d \theta}{(2+\cos \theta)^{2}}=\frac{2 \pi}{(\sqrt{3})^{3}}\\\ &\text { and so } \int_{0}^{2 \pi} \frac{d \theta}{(2+\cos \theta)^{2}}=\frac{4 \pi}{3 \sqrt{3}} \end{aligned}$$
Step-by-Step Solution
VerifiedKey Concepts
Contour Integrals
The purpose of changing a real integral into a contour integral is to utilize the properties of complex functions that make calculation easier, such as the Residue Theorem, which we'll discuss next.
When converting from real to complex integrals, variables are substituted. Here, the substitution \(z = e^{i\theta}\) transforms the integral from trigonometric to complex using the complex plane. You might picture the point \(z\) moving along the unit circle as \(\theta\) changes from 0 to \(2\pi\). This circle is our path of integration.
Understanding contour integration is not only beneficial for evaluating integrals but also provides insight into the profound connectivity between complex and real analysis. It opens up a rich toolbox for tackling otherwise challenging or unsolvable real integrals.
Residue Theorem
Residues can be thought of as the coefficients of the \((z - r)^{-1}\) term in the Laurent series expansion of a complex function. These play a critical role in determining the contribution of poles to the integral.
In the given problem, we identify the poles by factoring the denominator \(z^2 + 2az + 1\) into \( (z - r_1)(z - r_2) \). We then find that the pole \(r_1\) is inside the unit circle and use the Residue Theorem to calculate the integral.
It's calculated by evaluating the residue at \(r_1\), which corresponds to: \[\text{Res}(f(z), r_1) = \frac{a}{4(\sqrt{a^2 - 1})^3} \]
Finally, applying the Residue Theorem: \[ \oint_{C} \frac{z}{\left(z-r_{1}\right)^{2}\left(z-r_{2}\right)^{2}} \ dz = 2 \pi i \frac{a}{4(\sqrt{a^2 - 1})^3} \]
Understanding this theorem empowers one to simplify complex integrations significantly, making it fundamental not only in analysis but also in physics and engineering.
Trigonometric Integrals
In the exercise, we start with a trigonometric integral of the form:
\[ \int_{0}^{\pi} \frac{d \theta}{(a+\cos \theta)^{2}} \]
Trigonometric functions like cosine have periodic patterns, and this pattern influences the integral's evaluation. The integral presented is complex due to the composition \((a + \cos \theta)^2\).
Combining trigonometric and complex analysis by converting cosine to its exponential form through the substitution \(z = e^{i\theta}\) helps rectify the periodic difficulty. The substitution is done by expressing \(\cos \theta\) as \(\frac{z + z^{-1}}{2}\).
Ultimately, solving trigonometric integrals with these methods not only provides exact values for seemingly intractable integrals but also enhances one's toolkit for mathematical and practical problem-solving in fields such as physics, engineering, and signal processing.