The Fourier series expansion of the function $f(x) = |\cos(x)|$ in the interval $(-\pi, \pi)$ is $\alpha + \beta \left[ \frac{1}{3}\cos(2x) - \frac{1}{15}\cos(4x) + \dots \right]$. The values of $\alpha$ and $\beta$ respectively are ______.
We need to find the Fourier series for $f(x) = |\cos(x)|$ on $(-\pi, \pi)$. The function $f(x) = |\cos(x)|$ is an even function.
The general Fourier series for an even function is:
$f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} a_n \cos(nx)$
The provided series form is $\alpha + \beta \left[ \frac{1}{3}\cos(2x) - \frac{1}{15}\cos(4x) + \dots \right]$. Comparing this with the standard form, we identify $\alpha = \frac{a_0}{2}$ (the constant term) and $\beta$ is a factor related to the subsequent cosine coefficients.
First, compute $a_0$, which is the average value of $f(x)$ over the interval multiplied by $\pi$. Specifically, $a_0 = \frac{1}{\pi} \int_{-\pi}^{\pi} |\cos(x)| dx$. Since the function is even, we can write:
$a_0 = \frac{2}{\pi} \int_{0}^{\pi} |\cos(x)| dx$
The integral needs to be split because $\cos(x)$ changes sign at $x = \pi/2$:
$a_0 = \frac{2}{\pi} \left[ \int_{0}^{\pi/2} \cos(x) dx + \int_{\pi/2}^{\pi} (-\cos(x)) dx \right]$
Evaluate the integrals:
$a_0 = \frac{2}{\pi} \left[ [\sin(x)]_{0}^{\pi/2} - [\sin(x)]_{\pi/2}^{\pi} \right]$
$a_0 = \frac{2}{\pi} \left[ (\sin(\pi/2) - \sin(0)) - (\sin(\pi) - \sin(\pi/2)) \right]$
$a_0 = \frac{2}{\pi} \left[ (1 - 0) - (0 - 1) \right] = \frac{2}{\pi} (1 + 1) = \frac{4}{\pi}$
The constant term $\alpha$ is half of $a_0$:
$\alpha = \frac{a_0}{2} = \frac{1}{2} \left( \frac{4}{\pi} \right) = \frac{2}{\pi}$
Next, consider the cosine coefficients $a_n$. For $n \ge 1$, $a_n = \frac{1}{\pi} \int_{-\pi}^{\pi} |\cos(x)| \cos(nx) dx$. Due to symmetry, this simplifies to $a_n = \frac{2}{\pi} \int_{0}^{\pi} |\cos(x)| \cos(nx) dx$.
It can be shown that $a_n = 0$ for all odd integers $n$. For even integers $n=2k$ where $k \ge 1$, the coefficients are:
$a_{2k} = \frac{4(-1)^k}{\pi(1-4k^2)}$
Calculate the specific coefficients needed for the series structure:
The Fourier series begins:
$f(x) = \frac{a_0}{2} + a_2 \cos(2x) + a_4 \cos(4x) + \dots$
$f(x) = \frac{2}{\pi} + \frac{4}{3\pi} \cos(2x) - \frac{4}{15\pi} \cos(4x) + \dots$
Rewrite this by factoring out $\frac{4}{\pi}$ from the cosine terms:
$f(x) = \frac{2}{\pi} + \frac{4}{\pi} \left[ \frac{1}{3}\cos(2x) - \frac{1}{15}\cos(4x) + \dots \right]$
Comparing this calculated series $ \frac{2}{\pi} + \frac{4}{\pi} \left[ \dots \right] $ with the given form $ \alpha + \beta \left[ \dots \right] $, we identify:
$\alpha = \frac{2}{\pi}$
$\beta = \frac{4}{\pi}$
Thus, the values are $\alpha = \frac{2}{\pi}$ and $\beta = \frac{4}{\pi}$.
The Fourier series representation of a square wave is shown in the figure below. The fluctuations seen near $x = \pm 1$ are named after which one of the following scientists?

Periodic function $f(x)$ is given below. $$f(x) = \begin{cases} -1, & \text{when } -\pi < x < 0 \\ 1, & \text{when } 0 < x < \pi \end{cases} ; f(x + 2\pi) = f(x)$$ The CORRECT option representing the Fourier series expansion of $f(x)$ is:
A time-limited waveform $g(x)$ is specified as follows: $$g(x) = \begin{cases} -k, & -\pi < x \le 0 \\ +k, & 0 < x \le \pi \\ 0, & \text{otherwise} \end{cases}$$ A new waveform $f(x)$ is constructed from $g(x)$ as follows: $$f(x) = \sum_{m=-\infty}^{\infty} g(x + 2\pi m), \quad \text{for all } x \in \mathbb{R}$$ The sum of the coefficients of the third harmonics of the sine and cosine terms in the trigonometric Fourier series expansion of $f(x)$ is $\frac{2}{3\pi}$.
What is the value of $k$?
The effective value of the current for the Sawtooth waveform as shown is:

For fourier series of wave shown in Figure below,
Select correct expression for f(t)
