Frequency Modulation
Oct 26, 2014
Frequency Modulation
Relationship between FM and PMRelationship between FM and PM
• We can generate FM signal by using PM modulator and vice versa.
• From the above block diagrams, it can be shown that the generation of FM and PM signals are mutually related.
DifferentiatorFM
Modulatorvm(t) vPM(t)
dt
d
PMModulator
vm(t) vFM(t)Integrator
dtGeneration of FM
Generation of PM
)](cos[)( tvktEtv mpccPM
t
mfccFM dttvktEtv0
cos
• Demodulation process is used to get back the information signal.
• For FM demodulator in order to get back information signal from FM signal : PM modulator is used and the signal is pass through differentiator.
• In contrast for PM demodulator : FM demodulator is used and the signal is pass through the integrator.
• This shows the close relationship between FM and PM.
• Hence we can discuss only either one technique in angle modulation.
Differentiator
dt
dPM
Demodulatorvm(t)vFM(t)
FM Demodulator
FMDemodulator
vm(t)vPM(t) Integrator
dt
PM Demodulator
t
mfccFM dttvktEtv0
cos
)](cos[)( tvktEtv mpccPM
FM: Modulation Index
• Any modulation process produces sidebands.
• Side frequencies are the sum and difference of the carrier and modulating frequency.
• The bandwidth of an FM signal is usually much wider than that of an AM signal with the same modulating signal. (infinite number of pairs of upper and lower sidebands generate)
Modulation Index
– The ratio of the frequency deviation to the modulating frequency is known as the modulation index (m).
– In most communication systems using FM, maximum limits are put on both the frequency deviation and the modulating frequency.
)(
)(
Hzf
Hzfm
m
mm f
fm
mcmcmc nffffff ,2,
e.g. for m = 5,16 sidebands (8 pairs).
Determining the Number of Significant Sidebands
Bessel Functions – A complex mathematical process to
determining the number of significant sidebands
– The individual frequency components that make-up the modulated wave are not obvious. However, Bessel Function identities can be applied for this.
Bessel Function• Modulating wave is given by:
• By using Bessel Function, the angle-modulated wave can be written as:
• Jn(m) is the Bessel function of the first kind of nth order with argument m.
cos cos cos2n
n
nm J m n
)]cos(cos[)( tmtVtm mcc
• Thus, m(t) can be rewritten as
• Expanding the equation, becomes
• Where m = modulation index
Vc = peak amplitude of the unmodulated carrier
J0(m)= carrier component
J1(m)=first set of side frequencies displaced from the carrier by ωm
J2(m)=second set of side frequencies displaced from the carrier by 2ωm
Jn(m)=nth set of side frequencies displaced from the carrier by nωm
nmcmc
ntntmJVtm
2cos)()(
)...(.......)cos()(
)2cos()(]2
)cos[()(
]2
)cos[()(cos)()(
2
21
10
mJntmJ
tmJtmJ
tmJtmJVtm
mc
mcmc
mccc
Magnitudes of sidebands includes upper and lower sidebands are defined by J1(m), J2(m), and so on
• J can be defined as:
120) 5 4 3 2 1 Means5! (e.g.
index modulation m
frequency side theofnumber or J n
etc.)(1x2x3x4, factorial! where
...)!1(!3
62/
)!2(!2
42/
)!1(!1
2/1
2)(
2
n
m
n
m
n
m
n
mmJ
Figure 5-8: Carrier and sideband amplitudes for different modulation indexes of FM signals based on the Bessel functions.
Sidebands (Pairs)
Bessel Function PlotBessel Function Plot
Figure 5-9: Plot of the Bessel function data from Fig. 5-8.
Bessel Function PlotBessel Function Plot
Bessel Function PlotBessel Function Plot
Bandwidth
FM Signal Bandwidth– The higher the modulation index in FM, the greater the
number of significant sidebands and the wider the bandwidth of the signal.
– When spectrum conservation is necessary, the bandwidth of an FM signal can be restricted by putting an upper limit on the modulation index.
– E.g: In standard FM broadcasting, the maximum permitted frequency deviation is 75 kHz and the maximum permitted modulating frequency is 15 kHz (modulation index : 5)
Determining the Number of Significant Sidebands
mc mc c
m = 0.25
)( 1rads
BW
mc 4 mc 4c
m = 2
)( 1rads
BW=2nfm=8fm
mc 8 mc 8c
m = 5
)( 1rads
BW=2nfm=16fm
The number of sidebands depend on m value:
BW = 2fmNWhere N is the number of
significant* sidebands
*Significant sidebands are those that have an amplitude of greater than 1% (.01) in the Bessel table.
Bandwidth
Example:If the highest modulating frequency is 3 kHz and
the maximum deviation is 6 kHz, what is the modulation index?
m = 6 kHz/3 kHz = 2
What is the bandwidth?
BW = 2fmN
Where N is the number of significant* sidebands
BW = 2(3 kHz)(4) = 24 kHz
Solution:
Carlson’s RuleCarlson’s Rule
• Take into consideration only the power in the most significant sidebands whose amplitude are greater than 2 percent of the carrier (sidebands whose values are 0.02 or more)
• Therefore the BW needed for FM was :
maxmax2 mffBW
For FM Modulator with frequency deviation of 10 kHz, modulating frequency of 10 kHz, Carrier amplitude voltage of 10V and Carrier frequency of 500 kHz, determine the following:
(a) Minimum Bandwidth using Bessel table
(b) Minimum Bandwidth using Carson’s rule
(c) Amplitudes of the side frequencies and plot the output frequency spectrum
EXAMPLE 2 :
Solution:
a)
From Bessel function table, m=1 yields three sets of significant sidebands. Thus bandwidth is
b) Approx. minimum bandwidth is given by Carson’s rule. So
1kHz10
kHz10
mf
fm
Hz60)103(2 kkHzB
Hz40)1010(2 kkHzkHzB
c)
VJ
VJ
VJ
VJ
2.0)10(02.0
1.1)10(11.0
44)10(44.0
7.7)10(77.0
3
2
1
0
7.7V
44V
1.1V
0.2V
500 510 520 530490480470
0.2V
44V
1.1V
• Frequency spectrum consists of carrier component at fc and also sideband at fc±nfm where n is an integer (n = 1,2,3,…)
• The number of sideband depends on index modulation value, m.
• Magnitude of carrier signal decreases as m increases. • Amplitude of the frequency spectrum depends on
value of Jn(m).
• The bandwidth of modulated signal increases when index modulation, m increases. BW > 2∆fm is expected.
Summary of FM spectrum:
Power in FM signalPower in FM signal• Power signal depends on the amplitudes and not on the
frequencies. • The amplitude of the FM signal is constant and therefore the
power transmitted depends only on the amplitudes of the signal. It does not depends on the modulation index.
• For AM signal the power transmitted depends on the modulation index.
• It can be seen from the Bessel equation:
• In other word the total power of FM signal consists of the power in carrier component and all the power in the sidebands.
1
2
...2
0
3210
nJJ
JJJJJT
n
n
PP
PPPPPP
1
220
223
22
21
20 122...222
nnn JJJJJJJ
• FM equation is given by:
• And therefore the total power transmitted :
1
220
2
2223
222
221
220
2
2)(
2)(
2)(
2)(
2)(
)(
22
2...
2222
2
...2
...2
3210
3210
nn
c
nccccc
rmsJrmsJrmsJrmsJrmsJ
JJJJJFMT
JJR
E
R
JE
R
JE
R
JE
R
JE
R
JE
R
V
R
V
R
V
R
V
R
V
PPPPPP
n
n
])cos())[cos((...
])3cos()3)[cos((
])2cos()2)[cos((
])cos())[cos(()cos()()(
3
2
10
tntnJ
ttJ
ttJ
ttJtJEtv
mcmcn
mcmc
mcmc
mcmcccFM
Power Calculation
• The average power of modulated wave is defined as :
Pc = Vc2 / 2R
Vc=peak unmodulated carrier voltage (V)R = load resistance
The instantaneous power for angle modulation is defined as:Pt = m(t)2 / R W
or Pt = Vc
2 / R [1/2 +½ cos(2ωct + 2(t)]
• Average power of the second term is zero. Thus
Pc = Vc2 / 2R
Modulated carrier power = power of carrier + power of side frequency components
average power of modulated carrier = average power of unmodulated carrier.
Consists of an infinite number of sinusoidal
side frequency components
Power Calculation
• The total power for modulated wave is defined as:
• P0= modulated carrier power
• P1= power in the first set of sidebands
• P2= power in the second set of sidebands
• Pn= power in the nth set of sidebands
R
V
R
V
R
V
R
VP nct 2
)(2...
2
)(2
2
)(2
2
222
21
2
nt PPPP ...21
Narrowband and Wideband FM
From the graph/table of Bessel functions it may be seen that for small , ( 0.3) there is only the carrier and 2 significant sidebands, i.e. BW = 2fm.
FM with 0.3 is referred to as narrowband FM (NBFM) (Note, the bandwidth is the same as DSBAM).
For > 0.3 there are more than 2 significant sidebands. As increases the number of sidebands increases. This is referred to as wideband FM (WBFM).
Narrowband FM NBFM
Wideband FM WBFM
• Large modulation index m
c
f
f means that a large bandwidth is required – called
WBFM.
Narrow Band FM (NBFM)Narrow Band FM (NBFM)
• For FM signal with the small index modulation i.e m < 0.2, is called Narrow Band FM (FM jalur sempit)
• For FM signal that we have studied previously also known as WBFM and the equation is given by :
• Let :
• Hence, the equation yields:
• NBFM with m = small , therefore;
)sin(m)( tt m
)](sinm[sin)sin()]sin(mcos[)cos()( ttEttEtv mccmccFM
)]([sin)sin()](cos[)cos()( ttEttEtv ccccFM
1)sin(m)( tt m
])cos[(2
m])cos[(
2
m)cos(
)sin()sin(m)cos(
)sin()()cos()(
tE
tE
tE
ttEtE
ttEtEtv
mcc
mcc
cc
cmccc
ccccFM
1)](cos[ t )()](sin[ tt and
tmEt
mEtEtam mc
cmc
cccFCDSB cos
2cos
2cos)(
• Therefore :
• Hence NBFM equation yields :
• Compared with amDSB-FC signal:
• It is shown from both equations for NBFM and amDSB-FC consist of one carrier component and two sidebands components. But LSB component for NBFM the phase shift is varies for 90° (quadrature).
1)sin(m)( tt m
Differences between FM and AMDifferences between FM and AM
• Frequency spectrum)(VAmplitud
)( 1radsc mc mc 0
cA
2cmA
2cmA
22mc AmA
Di mana
)(VAmplitud
)( 1radsc mc mc 0
cA
2
cA
2
cA
AM FM
Figure: Carrier and sideband amplitudes for different modulation indexes of FM signals based on the Bessel functions.
Sidebands (Pairs)
Bessel Function PlotBessel Function Plot
Ex. 1 :
A carrier with a peak value of 2000 V is frequency modulated with a message signal of 5 kHz. The modulation index obtained is 2. Calculate the average power in:
(i) Highest sideband (ii) Lowest sideband . Given R = 50 Ω .
Solution : (β =m)
For β = 2 from Bessel table :
The highest sideband is : 58.01 JThe lowest sideband is : 01.05 J
03.02
58.02
4
1
J
J
=>
R
EP C 1
2
58.02
1
(i)
kW 5.1350
1
2
200058.02
50
1
2
200003.02
5
P
W4
(ii)
Ex. 2 :
(a) Determine the BW required to transmit FM signal when the modulating frequency, fm = 10 kHz and maximum frequency deviation is 20 kHz.
From Bessel table the components obtained is J0 , J1 , J2 , J3 , J4 and J5 That means J1 will be at 10 kHz, J2 at 20 kHz, J3 at 30 kHz etc.
Therefore BW = BFM = 2nfm = 2 x 5 x 10 = 100 kHz
210
20
mf
f
Amplitud
fc fc+fm fc+2fm
J0
J1
J5
fc-fm
f (kHz)
m
m
fffBW
212
Carson Rule
Solution :
(b) Repeat (a) with fm = 5 kHz
From Bessel table the highest component is J7
Therefore BW = 2 x 7 x 5 = 70 kHz
45
20
mf
f
m
m
fffBW
212
Carson Rule
Solution :
Equation for NBFM:
t
mfccFM dttvktEtv0
cos
Given, , tfEtv mmm 2sin kHz 10fkV 100cE
kHz 5dan V 1 , MHz 2.106 mmc fEf
(i) frequecy deviation
(ii) BW by Carson rule
(iii)Total Power
(iv)Equation for NBFM
Penyelesaian :
tfdttvkEtfEv
R
EP
ffBWf
f
Ekf
cmfcccNBFM
cFM
mm
mf
2sin22cos (iv)
1R gConsiderin ;kW 512
100
2 (iii)
kHz 3051022 25
10 (ii)
kHz 10110 (i)
22
)sin()(sin)cos()( ttEtEtv cmcccNBFM
Ex. 3 :
A FM signal, 2000 cos (2π x 108 t + 2 Sin π x 104t) is transmitted using an antenna with the resistance of 50 Ω. Determine
(i) Carrier frequency (ii) Modulation index (iii) Information signal
(iv) Power transmitted (v) Bandwidth (vi) Power in highest and lowest sidebandsPenyelesaian :
]sin[cos)( ttEtv mccFM
(i) fc = 108 Hz = 100 MHz
(ii) β = 2
(iii)fm = 104 / 2 = 5 kHz
i) (v) β = 2 => sideband 4
BW = BFM = 2nfm = 2 x 4 x 5 = 40 kHz
Carson - BW = 2(β + 1)fm = 2(2 + 1)5 = 30 kHz
i) (iv) Ec = 2000 V => Ec(rms) = 2000 / 2
PT = V2 (rms)
/ R
= (2000 / 2)2 / 50
= 40 kW
(vi) lowest side band J1 amplitude
for 1st side band = 0.58 x 2000
P = (0.58 x 2000/2)2 / 50 Ω
= 13.27 kW lowest sideband
For double side band
= 2 x 13.27 kW = 26.54 kW
Band limit : fc fm = 100 MHz 5 kHz
Highest sideband J4
P = (0.03 x 2000/2)2 / 50 Ω = 36 W