Chapter 7: Problem 5
Determine the Fourier series for the function defined by $$ \begin{aligned} f(x) &=2 x \quad 0 \leq x \leq 2 \pi \\ f(x+2 \pi) &=f(x) & \end{aligned} $$
Short Answer
Expert verified
The Fourier series is \( f(x) = 2 + \sum_{n=1}^{\infty} \frac{4}{n} \sin(nx)\)
Step by step solution
01
Write the Fourier series formula
The Fourier series for a function defined on [0, 2\pi] and periodic with period 2\pi is given by\(f(x) = a_0 + \sum_{n=1}^{\infty} (a_n \cos(nx) + b_n \sin(nx))\)
02
Compute the coefficient a_0
The coefficient a_0 is computed using:\(a_0 = \frac{1}{2\pi} \int_{0}^{2\pi} f(x) \text{d}x\)Substitute f(x) = 2x to get:\(a_0 = \frac{1}{2\pi} \int_{0}^{2\pi} 2x \text{d}x = \frac{2}{2\pi} [\frac{x^2}{2}]_{0}^{2\pi} = \frac{1}{\pi} [\pi^2] = 2\)
03
Compute the coefficients a_n
The coefficients a_n are computed using:\(a_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \cos(nx) \text{d}x\)Substitute f(x) = 2x to get:\(a_n = \frac{2}{\pi} \int_{0}^{2\pi} x \cos(nx) \text{d}x\)Using integration by parts, let u = x\ and \text{d}u = \cos(nx)\text{d}x\ to get:\(a_n = \frac{2}{\pi} [\frac{x\sin(nx)}{n}]_{0}^{2\pi} - \frac{2}{\pi} \int_{0}^{2\pi} \frac{\sin(nx)}{n} = 0\text{} \text{(since both terms integrate to zero over}[0, 2\pi] ) = 0\)
04
Compute the coefficients b_n
The coefficients b_n are computed using:\(b_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \sin(nx) \text{d}x\)Substitute f(x) = 2x to get:\(b_n = \frac{2}{\pi} \int_{0}^{2\pi} x \sin(nx) \text{d}x\)Using integration by parts, let u = x and dv = \text{sin} (nx )\text{d}x to get:\(b_n = -\frac{2}{n} [x \text{cos} (nx)]_{0}^{2\pi} + \frac{2}{n} \int_{0}^{2\pi} \text{cos} (nx) \text{d}x) = \frac{4}{n}\text{ (since the second term integrates to zero over}[0, 2\pi] }\)
05
Write the Fourier series
Substitute a_0, a_n, b_n into the Fourier series formula to get:\( f(x) = 2 + \sum_{n=1}^{\infty}\left( 0 \cos(nx) + \frac{4}{n} \sin(nx)\right) = 2 + \sum_{n=1}^{\infty} \frac{4}{n} \sin(nx)\)
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Key Concepts
These are the key concepts you need to understand to accurately answer the question.
Periodic Functions
A periodic function repeats its values at regular intervals, called periods. In this problem, we consider the function defined as \(f(x)=2x\) over the interval \([0, 2\pi]\), with the periodic condition \(f(x+2\pi)=f(x)\). This means that after every interval of \(2\pi\), the function returns to its original value. Periodic functions are essential in Fourier analysis because they can be represented by a sum of sine and cosine functions, which are also periodic.
Fourier Coefficients
Fourier coefficients are the constants \(a_0\), \(a_n\), and \(b_n\) in the Fourier series. They are determined through integration and characterize the amplitude of the sine and cosine components of the function.
For our function:
For our function:
- The coefficient \(a_0\) is found using the integral \(a_0 = \frac{1}{2\pi} \int_{0}^{2\pi} f(x) \, \text{d}x\).
- The coefficients \(a_n\) and \(b_n\) are found using \(a_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \cos(nx) \, \text{d}x\) and \(b_n = \frac{1}{\pi} \int_{0}^{2\pi} f(x) \, \sin(nx)\text{d}x\) respectively.
Integration by Parts
Integration by parts is a technique used to integrate products of functions. It is based on the product rule for differentiation and is given by the formula: \[ \int u \, \text{d}v = uv - \int v \, \text{d}u \] For our problem, integration by parts is used twice:
- To find \(a_n\), set \(u = x\) and \(\text{d}v = \cos(nx)\text{d}x\).
- To find \(b_n\), set \(u = x\) and \(\text{d}v = \sin(nx)\text{d}x\).
Trigonometric Series
A trigonometric series is a sum of sine and cosine functions. The Fourier series is a type of trigonometric series used to represent periodic functions.
The general form of the Fourier series is: \[ f(x) = a_0 + \sum_{n=1}^{\infty} (a_n \cos(nx) + b_n \sin(nx)) \] For the given function, substituting the calculated Fourier coefficients, we obtain:
The general form of the Fourier series is: \[ f(x) = a_0 + \sum_{n=1}^{\infty} (a_n \cos(nx) + b_n \sin(nx)) \] For the given function, substituting the calculated Fourier coefficients, we obtain:
- \(a_0 = 2\)
- \(a_n = 0\) for all \(n\)
- \(b_n = \frac{4}{n}\)