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 expansion of x3 in the interval −1 ≤ x < 1 with periodic continuation has
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