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ECE 460: Communication and Information Theory
Prof. B.-P. Paris
Homework 2
Solution
![F [x(t) ⋆ y(t)] = F [x(t)]F [y(t)] = X (f)Y (f)](hwsol_46044x.png)
Thus
![-1
sinc(t) ⋆ sinc (t) = F [F [sinc (t) ⋆ sinc(t)]]
= F -1[F [sinc (t)] ⋅ F[sinc(t)]]
-1 -1
= F [Π (f)Π (f)] = F [Π (f)]
= sinc (t)](hwsol_46045x.png)
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![∫ ∞
F [x(t)y(t)] = x(t)y(t)e -j2πftdt
∫- ∞∞ (∫ ∞ )
= X (θ)ej2πθtdθ y(t)e -j2πftdt
-∞ - ∞( )
∫ ∞ ∫ ∞ -j2π(f-θ)t
= -∞ X (θ) -∞ y(t)e dt dθ
∫ ∞
= X (θ)Y (f - θ)dθ = X (f) ⋆ Y (f)
-∞](hwsol_46046x.png)
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However, this relation cannot hold since Π(f) = 0 for 1
2 < |f| whereas
Λ(f)
0 for 1 < |f|≤ 1∕2.
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![- 1
yl(t) = F [Yl(f)]
1-∫ 0 j2πft -1-∫ 12 j2πft
= 2j - 1(f + 1)e df + 2j 0 (- f + 1)e df
[ 2 ] | |
1-- -1--- j2πft --1---j2πft ||0 -1--1---j2πft||0
= 2j j2πtf e + 4π2t2e |- 1 + 2j j2πte |- 1
[ ] 2|1 |12
-1- -1--- j2πft --1---j2πft ||2 1---1-- j2πft||2
- 2j j2πtfe + 4π2t2e |0 + 2jj2πt e |0
[ 1 1 ]
= j - ----sin πt + -----(cos πt - 1)
4πt 4π2t2](hwsol_46051x.png)
![[ ]
y (t) = Re (j[- -1--sinπt + --1---(cosπt - 1)])(cos 2πf0t + j sin2πf0t )
4πt 4 π2t2
--1--- -1--
= [4π2t2(1 - cosπt) + 4πt sin πt]sin2πf0t](hwsol_46052x.png)
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