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:
The given function is:
$f(x) = \begin{cases} -1, & \text{when } -\pi < x < 0 \\ 1, & \text{when } 0 < x < \pi \end{cases} ; f(x + 2\pi) = f(x)$This function is defined over the interval $(-\pi, \pi)$ and is periodic with period $2\pi$. We observe that $f(-x) = -f(x)$, indicating that $f(x)$ is an odd function.
The formula for the sine coefficient $b_n$ is:
$b_n = \frac{1}{\pi} \int_{-\pi}^{\pi} f(x) \sin(nx) dx$Because $f(x)$ is an odd function and $\sin(nx)$ is also an odd function, their product $f(x)\sin(nx)$ is an even function. Therefore, the integral can be simplified:
$b_n = \frac{2}{\pi} \int_{0}^{\pi} f(x) \sin(nx) dx$In the interval $(0, \pi)$, $f(x) = 1$. Substituting this value:
$b_n = \frac{2}{\pi} \int_{0}^{\pi} (1) \sin(nx) dx$ $b_n = \frac{2}{\pi} \left[ -\frac{\cos(nx)}{n} \right]_{0}^{\pi}$ $b_n = -\frac{2}{n\pi} [\cos(n\pi) - \cos(0)]$Using $\cos(n\pi) = (-1)^n$ and $\cos(0) = 1$:
$b_n = -\frac{2}{n\pi} [(-1)^n - 1]$So, the non-zero coefficients occur only for odd values of $n$. The Fourier series becomes:
$f(x) = \sum_{n \text{ odd}, n\ge 1}^{\infty} \frac{4}{n\pi} \sin(nx)$ $f(x) = \frac{4}{\pi} \sum_{n \text{ odd}, n\ge 1}^{\infty} \frac{\sin(nx)}{n}$ $f(x) = \frac{4}{\pi} \left[ \sin x + \frac{\sin 3x}{3} + \frac{\sin 5x}{5} + \dots \right]$Comparing this result with the given options, the correct Fourier series expansion for $f(x)$ is:
$f(x) = \frac{4}{\pi} \left[ \sin x + \frac{\sin 3x}{3} + \frac{\sin 5x}{5} + \dots \right]$If we use the Fourier transform ϕ(x, y) = \(\int {{{\rm{e}}^{{\rm{ikx}}}}} {ϕ _{\rm{k}}}\left( {\rm{y}} \right){\rm{dk}}\) to solve the partial differential equation \({\rm{ - }}\frac{{{\partial ^2}ϕ \left( {x,y} \right)}}{{\partial {y^2}}}\, - \,\frac{1}{{{y^2}}}\frac{{{\partial ^2}ϕ \left( {x,y} \right)}}{{\partial {x^2}}} + \frac{{{m^2}}}{{{y^2}}}ϕ \left( {x,y} \right) = 0\) in the half-plane {(x, y) : -∞ < x < ∞, 0 < y < ∞} the Fourier modes ϕ k(y) depend on y as y α and y β . The values of α and β are
When a time-domain signal is converted into its Fourier representation, which of the following is/are conserved?
I. Energy
II. Power
The trigonometric Fourier series of a periodic time function can have
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The Fourier series to represent x-x2 for –π ≤ x ≤ π is given by \(x - {x^2} = \frac{{{a_0}}}{2} + \mathop \sum \limits_{n = 1}^\infty {a_n}cosnx + \mathop \sum \limits_{n = 1}^\infty {b_n}sinnx\)
The value of a0 (round off to two decimal places), is