cheat sheet communications
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8/18/2019 Cheat Sheet Communications
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Cheat Sheet: ECE 318Prepared by Walid Abediseid
1 Modulation Schemes (see Table below)
– Why Modulation? Make transmission more reliable.Reduce noise and interference. To facilitate channel as-signment and multiplexing.
– For DSB-LC: µ = |max f (t)|Ac represents the modula-tion index. In this case, one may rewrite the DSB-LC as: s(t) = Ac(1 + µf (t)) cos(ωc + φ), conditionedon |max f (t)| = 1. The modulation efficiency is de-
fined by η = P f /2P f /2+A2c/2
, or η = µ2P f /2µ2P f /2+1/2
= µ2P f 1+µ2P f
(for the other representation). A special case, is whenf (t) = cos(ωf t) or sin(ωf t). In this case, we have
P f = 1/2, and η = µ2
2+µ2 .
– For SSB: f̂ (t) = 1πt∗f (t) is the Hilbert Transform of f (t)(hard to find in time-domain). In frequency domain:
F̂ (ω) = − jsgn(ω)F (ω). Hilbert Transform acts as a90◦ phase delay. Example cos(ωt) = cos(ωt − π/2) =sin(ωt), in this case no need to do Fourier Transform.
– All the above modulation schemes can be demodulated(coherently) using the following:
s(t) ×
cos(ωct + φ)
LPF Acf (t)
However, for VSB modulation scheme, the filter at the
transmitter side hVSB(t) must satisfy the condition:H (ω−ωc) + H (ω + ωc) = constant, so that one can usethe above demodulator to recover the actual messagesignal f (t).
– An exception to the above demodulator, is the DSB-LC. If the modulation index µ such that the envelopeof s(t) is greater than zero, i.e., (Ac + µf (t)) > 0, thena simple RC circuit can be used to recover f (t).
2 Noise Filtering in LTI Systems
A random noise signal, n(t), is called white if it has a
power spectral density function, S n(ω), that is flat for
all frequencies, i.e., S n(ω) = K 2 where K is a consta
The average power of a signal x(t) with power spect
density S x(ω) is given by: P x = 12π
∞
−∞
S x(ω) dω a
since S x(ω) is a non-negative function, one can write above equation as P x =
12π × [Total Area under S x(ω
Signal-to-Noise Ratio (SNR) is defined by: SNR Average Power of Transmitted Signal
Average Power of Noise . The following pr
erty of LTI systems is very important:
r(t)
S r(ω)
LTI
H (ω)g(t) = r(t) ∗ h(t)
S g(ω) = S r(ω)|H (ω)|2
Example 1. Suppose we have r(t) = x(t) + n(t) is the into the above LTI system, where n(t) is a white noise wS n(t) = K/2, and
ω
S x(ω)
−2πB
1
2πBω
H (ω)
−πB
1/2
πB
Find the SNR at the output?
Solution: Let y(t) = x(t) ∗ h(t), and n(t) = n(t) ∗ h(t).order to find the average power of y(t) and n(t), we nto find their corresponding power spectral density functi
S y(ω), S n(ω):
ω
S y(ω)
−πB
1/4
1/8
πBω
S n(ω)
−πB
K/8
πB
In this case, the average power of y(t) can be eily evaluated using: P y =
12π [Area under S y(ω)]
12π [Area of rectangle +Area of triangle] =
316
B. Also, P n1
2π [2πB × K
8 ] = BK
8 . Therefore, the SNR=
3B/16
BK/8 = 3
2K .
Scheme Format Power P s Band-Width Bs
DSB-LC s(t) = (Ac + f (t)) cos(ωct + φ) A2c
2 + µ2P f
2 2Bf
DSB-SC s(t) = Acf (t) cos(ωct + φ) A2cP f
2 2Bf
USSB s(t) = Acf (t) cos(ωct + φ) − Ac f̂ (t)sin(ωct + φ) A2cP f
4 Bf
LSSB s(t) = Acf (t) cos(ωct + φ) + Ac f̂ (t)sin(ωct + φ) A2cP f
4 Bf
VSB s(t) = sDSB−SC(t) ∗ hVSB(t) depend on filter depend on filter
savals Thm: ∞−∞ x(t)y(t)
∗ dt = 12π ∞−∞ X (ω)Y (ω)
∗ dω. Averag power of x(t), P x = limT →∞1T
T/2−T/2 |x(t)|
2 dt. Power[C
=1 C k cos(ωkt + φk)] = C 20 +
nk=1
C 2k2 , where ωi = ωj for i = j . If the input to an LIT system with Frequency Response H (
he complex exponential A exp( jω0t) =⇒ the output is simply given by A|H (ω0)| exp( j[ω0t + ∠H (ω0)]). Autocorrelation of xt) = F −1{S x(ω)}. Average power also equal to Rx(0).