tele3113 wk6tue
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TELE3113 Analogue and DigitalCommunications
Transmission of FM Waves
Wei Zhang
School of Electrical Engineering and Telecommunications
The University of New South Wales
Wideband FM Signal
In the last lecture, we studied:
The FM wave of the single-tone message signal is given by
s(t) = Ac
∞∑
n=−∞
Jn(β) cos[2π(fc + nfm)t].
The spectrum of s(t) is given by
S(f) =Ac
2
∞∑
n=−∞
Jn(β)[δ(f − fc − nfm) + δ(f + fc + nfm)].
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.1/9
Transmission BW of FM (1)
In theory, an FM wave contains an infinite number of
side-frequencies, so the BW is infinite.
In practice, the FM wave is effectively limited to a finitenumber of significant side-frequencies.
Specifically, by observing the spectrum,
for large β, the BW approaches 2∆f = 2βfm.
for small β, the BW approaches 2fm.
Carson’s rule:
BT ≈ 2∆f + 2fm = 2∆f
(
1 +1
β
)
.
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.2/9
Transmission BW of FM (2)
Carson’s rule is simple, but not an accurate estimate.
An accurate estimate of the BW can be defined as the
separation between the two frequencies beyond whichnone of the side frequencies is greater than 1% of theunmodulated carrier amplitude.
Mathematically, the BW is given by (universal rule)
BT = 2nmaxfm = 2∆fnmax
β
where nmax is the largest value of the integer n that satisfies
|Jn(β)| > 0.01.
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.3/9
Transmission BW of FM (3)
β 0.1 0.3 0.5 1 2 5 10 20 30
2nmax 2 4 4 6 8 16 28 50 70
BT
∆f= 2nmax
β
10−1
100
101
100
101
102
Modulation index, β
Nor
mal
ized
ban
dwid
th, B
T/∆
f
BT/∆ f in term of β
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.4/9
Transmission BW of FM (4)
Relative error of BW estimate with Carson’s rule compared to
the universal rule is defined by
ε = 1 −BCarson
T
BUniversalT
=
(
1 −1 + β
nmax
)
× 100%.
Usually, Carson’s rule underestimates the BW by 25%.
10−1
100
101
−10
−5
0
5
10
15
20
25
30
35
40
Modulation index, β
Rel
ativ
e er
ror
of B
W e
stim
ate
(\%
)
Relative error of Carson’s rule in term of β
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.5/9
Generation of FM Waves (1)
Armstrong’s method:
The message signal is first used to produce a narrow-band
FM.
Then, a frequency multiplication is used to produce a
wide-band FM.
Integrator
Narrow-band phase Modulator
Message signal m(t) Wide-
band FM wave
Crystal controlled oscillator
Narrow-band phase modulator
Frequency multiplier
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.6/9
Generation of FM Waves (2)
Memoryless nonlinear
device
Bandpass filter with mid-band
frequency nfc
FM wave s(t) with carrier frequency fc
and modulation
�
FM wave s’ (t) with
carrier frequency nfc
and modulation
n
�
Frequency multiplier
v(t)
The input-output relation of the nonlinear device is
v(t) = a1s(t) + a2s2(t) + · · · + ansn(t),
where a1, a2, · · · , an are coefficients determined by the device
and n is the highest order of nonlinearity.
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.7/9
Generation of FM Waves (3)
Consider the input s(t) is an FM wave defined by
s(t) = Ac cos
[
2πfct + 2πkf
∫ t
0
m(τ)dτ
]
.
Suppose that bandpass filter is designed to have a BW
equal to n times the BW of s(t).
After bandpass filtering of the output v(t), we have
s′(t) = Ac cos
[
2πf′
ct + 2πk′
f
∫ t
0
m(τ)dτ
]
,
where f′
c = nfc and k′
f = nkf .
TELE3113 - Transmission of FM Waves. August 25, 2009. – p.8/9
Demodulation of FM Waves
Recall that the FM signal is given by
s(t) = Ac cos
[
2πfct + 2πkf
∫ t
0
m(τ)dτ
]
.
After taking the derivative of s(t) with respect to t, we get
ds(t)
dt= −2πAc[fc + kfm(t)] sin
(
2πfct + 2πkf
∫ t
0
m(τ)dτ
)
.
The derivative is indeed a band-pass signal with amplitudemodulation and the amplitude is 2πAcfc[1 + kfm(t)/fc].
If fc is large enough such that the carrier is not
overmodulated, then we can recover the message signal
m(t) with an envelop detection. TELE3113 - Transmission of FM Waves. August 25, 2009. – p.9/9