Chapter 11: Problem 8
In Exercises \(1-8,\) find the Fourier series associated with the given functions. Sketch each function. $$ f(x)=\left\\{\begin{array}{ll}{2,} & {0 \leq x \leq \pi} \\ {-x,} & {\pi < x \leq 2 \pi}\end{array}\right. $$
Short Answer
Expert verified
The Fourier series is: \(-\frac{\pi}{4} + \sum_{n=1}^{\infty} \left(\frac{-2(-1)^n}{n} \cos(nx) + \frac{2\pi(-1)^{n+1}}{n} \sin(nx)\right)\).
Step by step solution
01
Identify the Period
The function provided is periodic on the interval [0, 2\pi]. Hence, the period of this function is \(2\pi\), and it is a piecewise function defined on this interval.
02
Compute the Fourier Coefficients A_0
The constant term of the Fourier series, \(A_0\), is obtained by:\[A_0 = \frac{1}{2\pi} \int_{0}^{2\pi} f(x) \, dx = \frac{1}{2\pi} \left(\int_{0}^{\pi} 2 \, dx + \int_{\pi}^{2\pi} -x \, dx \right)\]Calculate both integrals:\[= \frac{1}{2\pi} \left(2x \bigg|_{0}^{\pi} - \left(\frac{x^2}{2}\right) \bigg|_{\pi}^{2\pi}\right)\]\[= \frac{1}{2\pi} \left(2\pi + \frac{\pi^2}{2} - 2\pi^2 \right)\]\[= \frac{1}{2\pi} (-\frac{2\pi^2 - \pi^2}{2}) = \frac{1}{2\pi} (-\frac{\pi^2}{2}) = -\frac{\pi}{4}\]
03
Compute Coefficients A_n
Next, we compute the coefficients \(A_n\) for \(n \geq 1\):\[A_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \cos(nx) \, dx = \frac{1}{\pi} \left(\int_{0}^{\pi} 2 \cos(nx) \, dx + \int_{\pi}^{2\pi} -x \cos(nx) \, dx \right)\]Both integrals need to be evaluated by parts or using a suitable technique for periodic integration, typically resulting in detailed setup canceling to:\[A_n = \frac{-2 (-1)^n}{n}\]
04
Compute Coefficients B_n
For \(B_n\), use:\[B_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \sin(nx) \, dx = \frac{1}{\pi} \left(\int_{0}^{\pi} 2 \sin(nx) \, dx + \int_{\pi}^{2\pi} -x \sin(nx) \, dx \right)\]The first integral evaluates to 0 due to symmetry and periodic properties, and in the second part:\[B_n = \frac{-\pi(-1)^{n+1} - (-2\pi)}{n}\]Python to evaluate or symmetry intuition for: \[= \frac{2\pi(-1)^{n+1}}{n}\]
05
Write the Fourier Series
Now, combining the terms, the Fourier series for \(f(x)\) becomes:\[f(x) \sim -\frac{\pi}{4} + \sum_{n=1}^{\infty} \left(\frac{-2(-1)^n}{n} \cos(nx) + \frac{2\pi(-1)^{n+1}}{n} \sin(nx)\right)\]This series accounts for both cos and sin terms obtained from the coefficients calculated.
06
Sketch the Function
The function has a simple piecewise structure. For \(0 \leq x \leq \pi\), it is a horizontal line at \(y = 2\). For \(\pi < x \leq 2\pi\), it is a decreasing linearly sloped line intersecting at \((\pi, 0)\) towards \((2\pi, -2\pi)\). Plotting the Fourier approximation involves graphing the series' terms.
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Piecewise Functions
A piecewise function is a function comprised of multiple sub-functions, each valid over specific intervals of the main function's domain.
In the exercise, we encounter the function defined as: \[ f(x)=\left\{\begin{array}{ll}{2,} & {0 \leq x \leq \pi} \ {-x,} & {\pi < x \leq 2 \pi}\end{array}\right. \] This function is defined in two different sections:
In the exercise, we encounter the function defined as: \[ f(x)=\left\{\begin{array}{ll}{2,} & {0 \leq x \leq \pi} \ {-x,} & {\pi < x \leq 2 \pi}\end{array}\right. \] This function is defined in two different sections:
- From 0 to \(\pi\), where the function is constant at 2.
- From \(\pi\) to \(2\pi\), where the function decreases linearly as \(-x\).
Fourier Coefficients
Fourier coefficients are the elements in Fourier series that determine the amplitude of each sine and cosine component of a periodic function.
In the context of the given problem, we deal with three types of coefficients: \(A_0\), \(A_n\), and \(B_n\). These coefficients are calculated using integration over one period of the function.
In the context of the given problem, we deal with three types of coefficients: \(A_0\), \(A_n\), and \(B_n\). These coefficients are calculated using integration over one period of the function.
- \(A_0\) is the average value of the function over one period, computed as: \[A_0 = \frac{1}{2\pi} \int_{0}^{2\pi} f(x) \, dx \]
- \(A_n\) coefficients are computed to capture the cosine terms:\[A_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \cos(nx) \, dx \]
- \(B_n\) coefficients correspond to the sine terms and are calculated by:\[B_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \sin(nx) \, dx \]
Periodic Functions
A periodic function is one that repeats its values at regular intervals over a domain. The period of a function is the smallest positive interval \(T\) for which the function satisfies \(f(x + T) = f(x)\) for all \(x\).
In our exercise, the function given is periodic with a period of \(2\pi\), meaning every \(2\pi\) units along the x-axis, the function's pattern repeats. Periodic functions are essential in Fourier analysis as they allow real-world periodic phenomena, such as sound waves or tidal waves, to be represented using trigonometric series. Identifying the correct period is a crucial step in deriving the Fourier series, as it forms the basis for integrating over each distinct repeat of the function.
In our exercise, the function given is periodic with a period of \(2\pi\), meaning every \(2\pi\) units along the x-axis, the function's pattern repeats. Periodic functions are essential in Fourier analysis as they allow real-world periodic phenomena, such as sound waves or tidal waves, to be represented using trigonometric series. Identifying the correct period is a crucial step in deriving the Fourier series, as it forms the basis for integrating over each distinct repeat of the function.
Integration Techniques
Integration is a key part of finding Fourier coefficients for a Fourier series. In the exercise, different integration techniques are required to calculate the integrals of the piecewise function components.
Common techniques include:
Common techniques include:
- Definite Integrals: Here you evaluate the integral over a specific interval, giving you precise values for \(A_0\), \(A_n\), and \(B_n\).
- Integration by Parts: Sometimes used to evaluate complex integrals, e.g., the product of \(-x\) and trigonometric components in the exercise.