The discrete-time Fourier series representation of a signal x[n] with period N is written as \(\rm x[n] = \sum_{k = 0}^{N - 1} a_k e^{j(2kn\pi/N)}\). A discrete-time periodic signal with period N = 3, has the non-zero Fourier series coefficients: a- 3 = 2 and a4 = 1. The signal is
The question asks for the representation of a discrete-time periodic signal $x[n]$ using its Discrete-Time Fourier Series (DTFS). The general formula for the DTFS representation is given as:
x[n] = \sum_{k = 0}^{N - 1} a_k e^{j \frac{2k n \pi}{N}}
Key information provided:
N = 3.a_{-3} = 2 and a_4 = 1.From the period N = 3, we know the fundamental frequency is $\omega_0 = \frac{2\pi}{N} = \frac{2\pi}{3}$.
A crucial property of DTFS coefficients is their periodicity with the same period as the signal. This means a_k = a_{k + mN} for any integer m.
We need to find the equivalent coefficients within the fundamental range k = 0, 1, ..., N-1 (which is k = 0, 1, 2 for N=3).
a_{-3}: Using the periodicity property, a_{-3} = a_{-3 \pmod{3}}. Since -3 is a multiple of 3, -3 mod 3 = 0. Thus, a_{-3} = a_0. Given a_{-3} = 2, we get a_0 = 2.a_4: Using the periodicity property, a_4 = a_{4 \pmod{3}}. Since 4 = 1*3 + 1, 4 mod 3 = 1. Thus, a_4 = a_1. Given a_4 = 1, we get a_1 = 1.Since only a_{-3} and a_4 are specified as non-zero, we infer that other coefficients within the fundamental period, like a_2, are zero.
Now we can reconstruct the signal $x[n]$ using the standard DTFS formula with the determined coefficients and fundamental frequency:
x[n] = \sum_{k=0}^{N-1} a_k e^{j k \omega_0 n}
For N=3, this expands to:
x[n] = a_0 e^{j \cdot 0 \cdot n \frac{2\pi}{3}} + a_1 e^{j \cdot 1 \cdot n \frac{2\pi}{3}} + a_2 e^{j \cdot 2 \cdot n \frac{2\pi}{3}}
Substituting the values a_0 = 2, a_1 = 1, and a_2 = 0:
x[n] = 2 \cdot e^{j \cdot 0} + 1 \cdot e^{j \frac{2\pi}{3} n} + 0
x[n] = 2 + e^{j \frac{2\pi}{3} n}
Let's simplify each option using Euler's formula \cos(\theta) = \frac{e^{j\theta} + e^{-j\theta}}{2} to see which one matches our derived signal x[n] = 2 + e^{j \frac{2\pi}{3} n}.
Note that the options use the frequency term $\frac{2\pi}{6} = \frac{\pi}{3}$.
Option 1: \rm 2 + 2e^{- \left( j \frac{2\pi}{6} n \right) }\cos \left( \frac{2 \pi}{6} n\right)
Simplifies to: 2 + 2e^{- j \frac{\pi}{3} n} \left( \frac{e^{ j \frac{\pi}{3} n} + e^{- j \frac{\pi}{3} n}}{2} \right) = 2 + 1 + e^{- j \frac{2\pi}{3} n} = 3 + e^{- j \frac{2\pi}{3} n}. This does not match.
Option 2: \rm 1 + 2e^{ \left( j \frac{2\pi}{6} n \right) }\cos \left( \frac{2 \pi}{6} n\right)
Simplifies to: 1 + 2e^{ j \frac{\pi}{3} n} \left( \frac{e^{ j \frac{\pi}{3} n} + e^{- j \frac{\pi}{3} n}}{2} \right) = 1 + e^{ j \frac{\pi}{3} n} e^{ j \frac{\pi}{3} n} + e^{ j \frac{\pi}{3} n} e^{- j \frac{\pi}{3} n} = 1 + e^{ j \frac{2\pi}{3} n} + 1 = 2 + e^{ j \frac{2\pi}{3} n}. This matches our derived signal.
Option 3: \rm 1 + 2e^{ \left( j \frac{2\pi}{3} n \right) }\cos \left( \frac{2 \pi}{6} n\right)
Simplifies to: 1 + 2e^{ j \frac{2\pi}{3} n} \left( \frac{e^{ j \frac{\pi}{3} n} + e^{- j \frac{\pi}{3} n}}{2} \right) = 1 + e^{ j \frac{2\pi}{3} n} e^{ j \frac{\pi}{3} n} + e^{ j \frac{2\pi}{3} n} e^{- j \frac{\pi}{3} n} = 1 + e^{ j \pi n} + e^{ j \frac{\pi}{3} n}. The frequency components here are incorrect for the DTFS sum with N=3.
Option 4: \rm 2 + 2e^{ \left( j \frac{2\pi}{6} n \right) }\cos \left( \frac{2 \pi}{6} n\right)
Simplifies to: 2 + 2e^{ j \frac{\pi}{3} n} \left( \frac{e^{ j \frac{\pi}{3} n} + e^{- j \frac{\pi}{3} n}}{2} \right) = 2 + e^{ j \frac{\pi}{3} n} e^{ j \frac{\pi}{3} n} + e^{ j \frac{\pi}{3} n} e^{- j \frac{\pi}{3} n} = 2 + e^{ j \frac{2\pi}{3} n} + 1 = 3 + e^{ j \frac{2\pi}{3} n}. This does not match.
Option 2, when simplified using Euler's formula, yields the expression 2 + e^{j \frac{2\pi}{3} n}. This corresponds to a DTFS representation with coefficients a_0 = 2 and a_1 = 1, which are consistent with the given non-zero coefficients a_{-3} = 2 and a_4 = 1 for a signal with period N = 3.
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
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), islet g(x) be a function defined by g(x) = x - [x], where [x] represents the integer part of x. (That is, it is the largest integer which is less than or equal to x). The value of the constant term in the Fourier series expansion of g(x) is ______.