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Prove that \(\int_{0}^{\infty} \frac{\sin x}{x} d x=\frac{1}{2} \pi\). [Hint: Let \(C\) be a path formed of the semicircular paths \(D_{r}:|z|=r\) and \(D_{R}:|z|=R\), where \(0 \leq \theta \leq \pi\) and \(0

Short Answer

Expert verified
A. \(\lim_{x\rightarrow 0}\int_{0}^{\infty} \frac{\sin x}{x} d x\) B. \(\lim_{r\rightarrow 0}\int_{a_r}^{r}\frac{e^{iz}-1}{z}dz\) C. \(\lim_{R\rightarrow \infty}\left\{\lim_{r\rightarrow 0} \oint_C\frac{e^{iz}}{z}dz\right\} - \pi i\) D. \(\int_{0}^{R}\frac{\sin x}{x}dx\)

Step by step solution

01

To show that \(\lim_{r\rightarrow 0}\int_{a_r}^{r}\frac{e^{iz}-1}{z}dz=0\), we first consider the modulus of the integral. We can write: $$\left|\int_{a_r}^{r}\frac{e^{iz}-1}{z}dz\right| \le \int_{a_r}^{r}\left|\frac{e^{iz}-1}{z}\right|dz$$ For \(|z|\le r\), we have \(|e^{iz}-1|\le |z|\) (using the well-known inequality \(|e^z-1|\le |z|\)). So, $$\int_{a_r}^{r}\left|\frac{e^{iz}-1}{z}\right|dz \le \int_{a_r}^{r}\frac{|z|}{|z|}dz = \int_{a_r}^{r}dz = r - a_r$$ Now, as \(r \rightarrow 0\), the difference \(r - a_r\) goes to zero. Therefore, the integral is zero: $$\lim_{r\rightarrow 0}\int_{a_r}^{r}\frac{e^{iz}-1}{z}dz = 0$$ #Step 2: Use Rule II and previous result to evaluate the integral#

Next, we use Rule II with the previous result and establish that: $$\lim_{R\rightarrow \infty}\left\{\lim_{r\rightarrow 0} \oint_C\frac{e^{iz}}{z}dz\right\} - \pi i = 0$$ This implies that: $$\lim_{R\rightarrow \infty}\left\{\lim_{r\rightarrow 0} \left[\int_{-R}^{-r} \frac{e^{ix}}{x}dx + \int_{r}^{R} \frac{e^{ix}}{x}dx\right] \right\} - \pi i = 0$$ #Step 3: Show that the imaginary part of the right-hand side has the value \(2\int_{0}^{\infty} \frac{\sin x}{x}dx - \pi\)#
02

Now, evaluate the imaginary part of the right-hand side. The imaginary part is given by: $$2 \operatorname{Im}\left[\int_{0}^{R}\frac{e^{ix}}{x}dx\right] - \pi$$ Recall that \(e^{ix}=\cos x +i\sin x\) and observe that its imaginary part is given by: $$\operatorname{Im}\left[\int_{0}^{R}\frac{e^{ix}}{x}dx\right] = \int_{0}^{R}\frac{\sin x}{x}dx$$ Thus, the imaginary part we are looking for is: $$2 \int_{0}^{\infty} \frac{\sin x}{x} d x - \pi$$ #Step 4: Finish the Proof#

Since the imaginary part of the right-hand side given in Step 3 has the value \(2 \int_{0}^{\infty} \frac{\sin x}{x} d x - \pi\), we can equate this to the right-hand side value: $$2 \int_{0}^{\infty} \frac{\sin x}{x} d x - \pi = 0$$ Therefore, $$\int_{0}^{\infty} \frac{\sin x}{x} d x = \frac{1}{2} \pi$$ The proof is complete, and the exercise has been solved.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Complex Analysis
At its core, complex analysis is the study of functions that operate on complex numbers. It is an area of mathematics mixing real and imaginary numbers, allowing us to consider dimensions that go beyond our real number scope. In complex analysis, we commonly deal with functions known as complex functions, which take on and return complex numbers. An essential tool in this field is the concept of the complex line integral, which helps us to integrate functions over contours in the complex plane. This is precisely where the Cauchy integral theorem finds its importance, as it provides conditions under which the complex line integral over a closed path is zero. This theorem is instrumental for solving integrals, such as the one in our exercise, and it's the groundwork for more advanced topics in complex analysis.
Contour Integration
Contour integration refers to the process of evaluating integrals along a path, or 'contour', in the complex plane. This process is not just about the path itself but more about understanding the function as you travel along this path. In mathematical terms, we are integrating a complex-valued function over a directed, smooth curve in the complex plane. To perform contour integration successfully, one needs to be familiar with the nature of the complex function being integrated and the properties of the contour. The Cauchy integral theorem plays a pivotal role here. It states that if a function is analytic (complex differentiable) everywhere within and on a simple closed contour, the integral over that contour is zero. This theorem simplifies the evaluation of many complex integrals and is fundamental in proving more complex propositions, like our sine integral exercise.
Sine Integral
The sine integral, denoted as \( Si(x) \), is a special function defined by the integral of the sine function divided by its argument, which is an example of a Fourier transform application. It is directly related to the problem we are solving: \( \int_{0}^{\infty} \frac{\sin x}{x} dx \). This type of integral appears in various areas of physics and engineering, such as signal processing and wave propagation. Solving it involves contour integration, where the function to be integrated is extended to the complex plane, allowing us to employ powerful tools from complex analysis, like the Cauchy integral theorem, and to navigate around singularities (points where the function is not defined).
Limit of an Integral
The concept of the limit of an integral is critical when dealing with improper integrals, where either the interval of integration is infinite or the function has an infinite discontinuity. In practice, taking the limit of an integral is closely linked to establishing its convergence and defining its value. In our exercise, we are interested in the limit of the sine integral as the argument tends to infinity, which is a classic improper integral scenario. Coupling the limit process with contour integration and the Cauchy integral theorem, we can cleverly manipulate the integral to serve our purposes and find its ultimate value, which, as we now know, turns out to be \( \frac{1}{2} \pi \). Understanding how limits interact with integrals is essential in various applications of both pure and applied mathematics.

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Most popular questions from this chapter

For each of the following, expand in a Laurent series at the isolated singularity given and state the type of singularity: a) \(\frac{e^{2}-1}{z}\) at \(z=0\) b) \(\frac{1}{z^{2}(z-3)}\) at \(z=0\) c) \(\frac{z-\cos z}{z}\) at \(z=0\) d) \(\csc z\) at \(z=0\) [Hint for (d): Write $$ \csc z=\frac{1}{\sin z}=\frac{1}{z-\left(z^{3} / 3 !\right)+\cdots}=\frac{a_{-1}}{z}+a_{0}+\cdots $$ and determine the coefficients \(a_{-1}, a_{0}, a_{1}, \ldots\) so that $$ \left.1=\left(z-z^{3} / 3 !+\cdots\right) \cdot\left(a_{-1} z^{-1}+a_{0}+a_{1} z+\cdots\right) \cdot\right] $$

(Cauchy's inequalities) Let \(f(z)\) be analytic in a domain including the circle \(C\) : \(\left|z-z_{0}\right|=R\) and interior and let \(|f(z)| \leq M=\) const on \(C\). Prove that $$ \left|f^{(n)}\left(z_{0}\right)\right| \leq \frac{M n !}{R^{n}} \quad(n=0,1,2, \ldots) . $$ [Hint: Apply (8.57).]

Evaluate each of the following with the aid of the Cauchy integral formula: a) \(\oint \frac{z}{z-3} d z\) on \(|z|=5\) b) \(\oint \frac{e^{*}}{z^{2}-3 z} d z\) on \(|z|=1\) c) \(\oint \frac{z+2}{z^{2}-1} d z\) on \(|z|=2\) d) \(\oint \frac{\sin z}{z^{2}+1} d z\) on \(|z|=2\) [Hint for (c) and (d): Expand the rational function in partial fractions.]

By means of (8.57), evaluate each of the following: a) \(\oint \frac{z e^{2}}{(z-1)^{4}} d z\) on \(|z|=2\) b) \(\oint \frac{\sin z}{z^{4}} d z\) on \(|z|=1\) c) \(\oint \frac{d z}{z^{2}(z+4)}\) on \(|z|=2\)

For each of the following, write the given function as two real functions of \(x\) and \(y\) and determine where the given function is continuous: a) \(w=(1+i) z^{2}\) b) \(w=\frac{z}{z+i}\) c) \(w=\tan z=\frac{\sin z}{\cos z}\) d) \(w=\frac{e^{-z}}{z+1}\) e) \(w=e^{z}\) f) \(w=\sin z\) g) \(w=\cos z\) h) \(w=\sinh z\) i) \(w=\cosh z\) j) \(w=e^{\tau} \cos z\)

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