Math Problem Statement

Fourier Series Expansion of f(x) = x/k in interval (0, 2 pi)

Solution

To find the Fourier Series expansion of the function f(x)=xkf(x) = \frac{x}{k} in the interval (0,2π)(0, 2\pi), we need to express the function as a sum of sine and cosine terms (for real Fourier series) or exponentials (for complex Fourier series). Let's start with the real Fourier series expansion.

Real Fourier Series Form

The Fourier series of a function f(x)f(x) defined on (0,2π)(0, 2\pi) is given by:

f(x)=a02+n=1(ancos(nx)+bnsin(nx))f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} \left( a_n \cos(nx) + b_n \sin(nx) \right)

Where the coefficients a0a_0, ana_n, and bnb_n are determined by the following integrals:

a0=1π02πf(x)dxa_0 = \frac{1}{\pi} \int_0^{2\pi} f(x) \, dx an=1π02πf(x)cos(nx)dxa_n = \frac{1}{\pi} \int_0^{2\pi} f(x) \cos(nx) \, dx bn=1π02πf(x)sin(nx)dxb_n = \frac{1}{\pi} \int_0^{2\pi} f(x) \sin(nx) \, dx

Step 1: Compute a0a_0

We start by computing a0a_0:

a0=1π02πxkdxa_0 = \frac{1}{\pi} \int_0^{2\pi} \frac{x}{k} \, dx

a0=1kπ02πxdx=1kπ[x22]02πa_0 = \frac{1}{k\pi} \int_0^{2\pi} x \, dx = \frac{1}{k\pi} \left[ \frac{x^2}{2} \right]_0^{2\pi}

a0=1kπ×(2π)22=2πka_0 = \frac{1}{k\pi} \times \frac{(2\pi)^2}{2} = \frac{2\pi}{k}

Thus:

a0=2πka_0 = \frac{2\pi}{k}

Step 2: Compute ana_n

Next, we compute ana_n:

an=1π02πxkcos(nx)dxa_n = \frac{1}{\pi} \int_0^{2\pi} \frac{x}{k} \cos(nx) \, dx

We can solve this integral using integration by parts. After computation, this integral evaluates to zero because it involves xcos(nx)x \cos(nx), which oscillates and cancels out over the interval (0,2π)(0, 2\pi).

Thus:

an=0for alln1a_n = 0 \quad \text{for all} \, n \geq 1

Step 3: Compute bnb_n

Finally, we compute bnb_n:

bn=1π02πxksin(nx)dxb_n = \frac{1}{\pi} \int_0^{2\pi} \frac{x}{k} \sin(nx) \, dx

Using integration by parts, we have:

bn=1kπ[xcos(nx)n02π+1n02πcos(nx)dx]b_n = \frac{1}{k\pi} \left[ -\frac{x \cos(nx)}{n} \Bigg|_0^{2\pi} + \frac{1}{n} \int_0^{2\pi} \cos(nx) \, dx \right]

The first term evaluates to zero because cos(nx)\cos(nx) at the limits 00 and 2π2\pi vanishes. The second integral also vanishes because it is the integral of a cosine over a full period (0,2π)(0, 2\pi).

Thus:

bn=2knb_n = \frac{2}{kn}

Final Fourier Series Expansion

Therefore, the Fourier series expansion of f(x)=xkf(x) = \frac{x}{k} in the interval (0,2π)(0, 2\pi) is:

f(x)=πk2kn=1(1)nnsin(nx)f(x) = \frac{\pi}{k} - \frac{2}{k} \sum_{n=1}^{\infty} \frac{(-1)^n}{n} \sin(nx)

This is the Fourier series expansion of f(x)f(x) in the given interval.

Would you like more details on any step?

Related Questions:

  1. What is the general formula for Fourier series expansion of any periodic function?
  2. How does changing the interval affect the Fourier series coefficients?
  3. How is the convergence of a Fourier series determined for a given function?
  4. What role do symmetry properties (odd/even) play in simplifying Fourier series?
  5. How can Fourier series be applied in solving partial differential equations?

Tip: Fourier series can help approximate complex waveforms by decomposing them into simpler trigonometric functions.

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Math Problem Analysis

Mathematical Concepts

Fourier Series
Trigonometric Functions
Integration by Parts

Formulas

f(x) = a_0/2 + ∑(a_n cos(nx) + b_n sin(nx))
a_0 = (1/π) ∫_0^2π f(x) dx
a_n = (1/π) ∫_0^2π f(x) cos(nx) dx
b_n = (1/π) ∫_0^2π f(x) sin(nx) dx

Theorems

Fourier Series Expansion Theorem
Orthogonality of Sine and Cosine

Suitable Grade Level

Undergraduate Mathematics