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If \(f(x)=\frac{1}{2} a_{0}+\sum_{1}^{\infty} a_{n} \cos n x+\sum_{1}^{\infty} b_{n} \sin n x=\sum_{-\infty}^{\infty} c_{n} e^{i n x},\) use Euler's formula to find \(a_{n}\) and \(b_{n}\) in terms of \(c_{n}\) and \(c_{-n},\) and to find \(c_{n}\) and \(c_{-n}\) in terms of \(a_{n}\) and \(b_{n}\).

Short Answer

Expert verified
Given \ f(x), \ a_{n} = c_{n} + c_{-n}, \ b_{n} = i (c_{n} - c_{-n}). \ c_{n} = \frac{a_{n}}{2} + \frac{ib_{n}}{2}, \ c_{-n} = \frac{a_{n}}{2} - \frac{ib_{n}}{2}.}

Step by step solution

01

- Recall Euler's Formula

Euler's formula states that for any real number \theta, \[ e^{i\theta} = \text{cos}(\theta) + i\text{sin}(\theta) \].Use this formula to express the cosine and sine functions in terms of exponentials.
02

- Rewrite f(x) Using Euler's Formula

Given\[ f(x) = \frac{1}{2} a_{0} + \text{sum}_{n=1}^{\text{∞}} a_{n} \text{cos}(nx) + \text{sum}_{n=1}^{\text{∞}} b_{n} \text{sin}(nx) \], rewrite \text{cos}(nx)\ and \text{sin}(nx)\ using Euler's formula:\[ \text{cos}(nx) = \frac{e^{inx} + e^{-inx}}{2}\] and \[ \text{sin}(nx) = \frac{e^{inx} - e^{-inx}}{2i}\].
03

- Substitute into the Series

Substitute the expressions for \text{cos}(nx)\ and \text{sin}(nx)\ into the original function:\[ f(x) = \frac{1}{2} a_{0} + \text{sum}_{n=1}^{\text{∞}} a_{n} \frac{e^{inx} + e^{-inx}}{2} + \text{sum}_{n=1}^{\text{∞}} b_{n} \frac{e^{inx} - e^{-inx}}{2i}\].
04

- Combine and Simplify the Series

Combine and simplify the series to match the exponential form \text{sum}_{n=-\text{∞}}^{\text{∞}} c_{n} e^{inx}:\[ f(x) = \frac{1}{2} a_{0} + \text{sum}_{n=1}^{\text{∞}} \frac{a_{n}}{2} (e^{inx} + e^{-inx}) + \text{sum}_{n=1}^{\text{∞}} \frac{b_{n}}{2i} (e^{inx} - e^{-inx})\].
05

- Equate Coefficients

Equate the coefficients of \text{each term} e^{inx} and e^{-inx}for the series \text{sum}_{n=-\text{∞}}^{\text{∞}} c_{n} e^{inx}. This gives us two equations:\[ c_{n} = \frac{a_{n}}{2} - \frac{b_{n}}{2i} = \frac{a_{n}}{2} + \frac{ib_{n}}{2} \] and \[ c_{-n} = \frac{a_{n}}{2} - \frac{b_{n}}{2i}\].
06

- Express Coefficients in Terms of Each Other

From the equations in step 5, solve for \ a_{n} \ and \ b_{n} \ in terms of \ c_{n} \ and \ c_{-n} \ :\[ a_{n} = c_{n} + c_{-n} \] and \[ b_{n} = i(c_{n} - c_{-n}) \].
07

- Final Expressions

Combine all the information to give:\[a_{n} = c_{n} + c_{-n}\] and \[ b_{n} = i (c_{n} - c_{-n})\]for \ c_{n} \ and \ c_{-n} \ we have:\[ c_{n} = \frac{a_{n}}{2} - \frac{b_{n}}{2i}\] and \[c_{-n}= \frac{a_{n}}{2} - \frac{b_{n}}{2i}\].

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Key Concepts

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

Euler's Formula
Euler's formula is a fundamental equation in complex analysis. It establishes a deeply insightful connection between complex exponentials and trigonometric functions. Euler's formula states that for any real number \theta\, the following relation holds:
\[ e^{i\theta} = \text{cos}(\theta) + i\text{sin}(\theta) \]
Here, \( e^{i\theta} \) represents a complex exponential, and the expression breaks down into a cosine term and an imaginary sine term.
This formula is especially useful because it allows us to convert trigonometric functions, like cosine and sine, into exponentials. For example:
\ e^{i nx} = \text{cos}(nx) + i \text{sin}(nx)\
and
\ e^{-i nx} = \text{cos}(nx) - i \text{sin}(nx)\

These relationships enable us to express trigonometric functions in exponential form, simplifying many calculations and derivations in the realm of signal processing and Fourier series.
Complex Exponentials
Complex exponentials provide a powerful way to handle periodic functions and signals in mathematics and engineering. They are especially useful in Fourier series, which decompose signals into their frequency components.
A complex exponential function is of the form \( e^{inx} \), where \ n \ is an integer, and \( x \) is a real variable.
Using Euler's formula, we can see that this function can be expressed as:
\[ e^{inx} = \text{cos}(nx) + i \text{sin}(nx) \]
Complex exponentials are crucial for transforming between time and frequency domains. For instance, in the Fourier series given in the problem, \( f(x) = \sum_{-\infty}^{\infty} c_n e^{inx} \), each term \( c_n e^{inx} \) represents a harmonic component of the signal.
Combining Euler’s formula with complex exponentials, we can convert between trigonometric and exponential forms of functions, which is essential in signal analysis.
Trigonometric Functions
Trigonometric functions, such as sine and cosine, are fundamental in describing periodic phenomena. They appear frequently in engineering, physics, and signal processing.
In the context of Fourier series, these functions are paramount. A Fourier series represents periodic functions as sums of sine and cosine terms. For instance, we have
\( \text{cos}(nx) \) and \( \text{sin}(nx) \) in
\ f(x) = \frac{1}{2} a_{0} + \sum_{n=1}^{\infty} a_{n} \cos(nx) + b_{n} \sin(nx) \.
Using Euler’s formula, we can express these trigonometric functions in terms of exponentials:
\[ \text{cos}(nx) = \frac{e^{inx} + e^{-inx}}{2} \]
and
\[ \text{sin}(nx) = \frac{e^{inx} - e^{-inx}}{2i} \]
This conversion is crucial for simplifying computations and solving complex problems. In the given exercise, this transformation makes it easier to find relationships between different coefficients in the Fourier series, bridging the gap between the time and frequency domains.

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Most popular questions from this chapter

You are given \(f(x)\) on an interval, say \(0< x< b\). Sketch several periods of the even function \(f_{c}\) of period \(2 b,\) the odd function \(f_{s}\) of period \(2 b,\) and the function \(f_{p}\) of period \(b\), each of which equals \(f(x)\) on \(0< x< b\). Expand each of the three functions in an appropriate Fourier series. $$f(x)=\left\\{\begin{array}{cl} x, & 0< x< 1 \\ 2-x, & 1< x< 2 \end{array}\right.$$

(a) Let \(f(x)\) on \((0,2 l)\) satisfy \(f(2 l-x)=f(x),\) that is, \(f(x)\) is symmetric about \(x=l .\) If you expand \(f(x)\) on \((0,2 l)\) in a sine series \(\sum b_{n} \sin \frac{n \pi x}{2 l},\) show that for even \(n, b_{n}=0 .\) Hint: Note that the period of the sines is \(4 l .\) Sketch an \(f(x)\) which is symmetric about \(x=l,\) and on the same axes sketch a few sines to see that the even ones are antisymmetric about \(x=l\). Alternatively, write the integral for \(b_{n}\) as an integral from 0 to \(l\) plus an integral from \(l\) to \(2 l,\) and replace \(x\) by \(2 l-x\) in the second integral. (b) Similarly, show that if we define \(f(2 l-x)=-f(x),\) the cosine series has \(a_{n}=0\) for even \(n\).

Given $$f(x)=\left\\{\begin{array}{cl}x, & 0 \leq x \leq 1 \\\2-x, & 1 \leq x \leq 2 \\\0, & x \geq 2 \end{array}\right.$$ find the cosine transform of \(f(x)\) and use it to write \(f(x)\) as an integral. Use your result to evaluate $$\int_{0}^{\infty} \frac{\cos ^{2} \alpha \sin ^{2} \alpha / 2}{\alpha^{2}} d \alpha.$$

Parts (a) and (b), you are given in each case one period of a function. Sketch several periods of the function and expand it in a sine-cosine Fourier series, and in a complex exponential Fourier series. (a) \(f(x)=x^{2},-\pi< x<\pi\) (b) \(f(x)=x^{2}, 0< x<2 \pi\)

In each of the following problems you are given a function on the interval \(-\pi < x < \pi\) Sketch several periods of the corresponding periodic function of period \(2 \pi\). Expand the periodic function in a sine-cosine Fourier series. $$f(x)=\left\\{\begin{array}{ll} 1, & -\pi < x < -\frac{\pi}{2}, \quad \text { and } \quad 0 < x < \frac{\pi}{2}; \\ 0, & -\frac{\pi}{2} < x < 0, \quad \text { and } \quad \frac{\pi}{2} < x < \pi. \end{array}\right.$$

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