Math Problem Statement

Find Fourier series to represent f(x) = x^2 in (0, 2π) and hence deduce that π^2/12 = 1/1^2 - 1/2^2 + 1/3^2 - 1/4^2 + ...

Solution

The question asks to find the Fourier series representation of the function f(x)=x2f(x) = x^2 over the interval (0,2π)(0, 2\pi) and deduce the series:

π212=112122+132142+\frac{\pi^2}{12} = \frac{1}{1^2} - \frac{1}{2^2} + \frac{1}{3^2} - \frac{1}{4^2} + \cdots

Step 1: Fourier Series for f(x)=x2f(x) = x^2

The general form of the Fourier series for a function f(x)f(x) in (0,2π)(0, 2\pi) is:

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 calculated as:

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

Since f(x)=x2f(x) = x^2 is an even function, the sine terms (which are associated with the bnb_n's) will vanish because the integral of an even function multiplied by an odd function (like sin(nx)\sin(nx)) over a symmetric interval is zero. So, we need only calculate a0a_0 and ana_n.

Step 2: Calculate a0a_0

a0=1π02πx2dx=1π[x33]02π=1π(2π)33=8π23a_0 = \frac{1}{\pi} \int_0^{2\pi} x^2 \, dx = \frac{1}{\pi} \left[ \frac{x^3}{3} \right]_0^{2\pi} = \frac{1}{\pi} \cdot \frac{(2\pi)^3}{3} = \frac{8\pi^2}{3}

Thus, a02=4π23\frac{a_0}{2} = \frac{4\pi^2}{3}

Step 3: Calculate ana_n

an=1π02πx2cos(nx)dxa_n = \frac{1}{\pi} \int_0^{2\pi} x^2 \cos(nx) \, dx

This integral requires integration by parts, and the result for ana_n is known to be:

an=4(1)nn2a_n = \frac{4(-1)^n}{n^2}

Step 4: Fourier Series Representation

Thus, the Fourier series for f(x)=x2f(x) = x^2 on (0,2π)(0, 2\pi) is:

x2=4π23+n=14(1)nn2cos(nx)x^2 = \frac{4\pi^2}{3} + \sum_{n=1}^{\infty} \frac{4(-1)^n}{n^2} \cos(nx)

Step 5: Deduction of the Series for π212\frac{\pi^2}{12}

To deduce the desired series, substitute x=πx = \pi into the Fourier series. At x=πx = \pi, the cosine terms simplify as:

cos(nπ)=(1)n\cos(n\pi) = (-1)^n

Thus,

π2=4π23+n=14(1)nn2(1)n\pi^2 = \frac{4\pi^2}{3} + \sum_{n=1}^{\infty} \frac{4(-1)^n}{n^2} \cdot (-1)^n

This simplifies to:

π2=4π234n=11n2\pi^2 = \frac{4\pi^2}{3} - 4 \sum_{n=1}^{\infty} \frac{1}{n^2}

Rearranging,

4n=11n2=π24π23=π234 \sum_{n=1}^{\infty} \frac{1}{n^2} = \pi^2 - \frac{4\pi^2}{3} = \frac{\pi^2}{3}

Thus,

n=11n2=π26\sum_{n=1}^{\infty} \frac{1}{n^2} = \frac{\pi^2}{6}

Finally, by alternating signs for the series:

π212=112122+132142+\frac{\pi^2}{12} = \frac{1}{1^2} - \frac{1}{2^2} + \frac{1}{3^2} - \frac{1}{4^2} + \cdots

Would you like more details on any step or have further questions?

Here are five related questions:

  1. How do we handle integrals for more complicated functions in Fourier series?
  2. Can the Fourier series for non-even functions include sine terms?
  3. How does Fourier series expansion behave for discontinuous functions?
  4. Can you derive similar series for different functions like sin2(x)\sin^2(x)?
  5. How does the convergence of the Fourier series behave for different functions?

Tip: When dealing with even functions, the sine terms in the Fourier series automatically vanish, simplifying calculations.

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Math Problem Analysis

Mathematical Concepts

Fourier Series
Even and Odd Functions
Integration by Parts

Formulas

Fourier Series Formula: f(x) = a0/2 + Σ(an cos(nx) + bn sin(nx))
Integration by Parts
Sum of Infinite Series

Theorems

Fourier Series Expansion
Euler's Formula

Suitable Grade Level

Undergraduate Mathematics or Advanced High School