1. NATIONAL COLLEGE OF SCIENCE AND TECHNOLOGY
Amafel Bldg. Aguinaldo Highway Dasmariñas City, Cavite
ASSIGNMENT # 3
“FREQUENCY MODULATION”
Cauan, Sarah Krystelle P. July 11, 2011
Communications 1 / BSECE 41A1 Score:
Eng‟r. Grace Ramones
Instructor

2. FREQUENCY MODULATION
Frequency Modulation Principles
While changing the amplitude of a radio signal is the most obvious method to modulate
it, it is by no means the only way. It is also possible to change the frequency of a signal to give
frequency modulation or FM. Frequency modulation is widely used on frequencies above 30
MHz, and it is particularly well known for its use for VHF FM broadcasting.
In FM, the carrier amplitude remains constant, while the carrier frequency is changed by
the modulating signal. As the amplitude of the information signal varies, the carrier frequency
will shift in proportion. As the modulating signal amplitude increases, the carrier frequency
increases. If the amplitude of the modulating signal, decreases the carrier frequency decreases.
The reverse relationship can also be implemented. A decreasing modulating signal will increase
the carrier frequency above its center value, whereas an increasing modulating signal amplitude
varies, the carrier frequency varies above and below its normal center frequency with no
modulation. The amount of change in carrier frequency produced by the modulating signal is
known as the frequency deviation. Maximum frequency deviation occurs at the maximum
amplitude of the modulating signal.
The frequency of the modulating signal determines how many times per second the
carrier frequency deviates above and below its nominal center frequency. If the modulating
signal is 100-Hz sine wave, then the carrier frequency will shift above and below the center
frequency 100 times per second. This is called the frequency deviation rate.
An FM signal is illustrated in Figure 1. With no modulating signal applied, the carrier
frequency is a constant-amplitude sine wave at its normal constant center frequency.
The modulating information signal is a low-frequency sine wave. As the sine wave goes
positive, the frequency of the carrier increases proportionately. The highest frequency occurs at
the peak amplitude of the modulating signal. As the modulating signal amplitude decreases, the
carrier frequency decreases. When the modulating signal is zero amplitude, the carrier will be at
its center frequency point.

3. Now when the modulating signal goes negative, the carrier frequency will decrease. The
carrier frequency will continue to decrease until the peak of the negative half cycle of the
modulating sine wave is reached. Then, as the modulating signal increases toward zero, the
frequency will again increase. Note in Figure 1 how the carrier sine waves seem to be first
“compressed” and then “stretched” by the modulating signal.
a)
b)
c)
Figure 1 The principle of frequency modulation: (a) carrier signal, (b) modulating signal
(c) Modulated signal (Frequency Modulation)

4. Phase Modulation
Another way to produce angle modulation is to vary the amount of phase shift of a
constant frequency carrier in accordance with a modulating signal. The resulting output is a PM
signal. Imagine a modulator circuit whose basic function is to produce a phase shift. Remember
that a phase shift refers to a time separation between two sine waves of the same frequency.
Assume that we can build a phase shifter that causes the amount of phase shift to vary with the
amplitude of the modulating signal. The greater the amplitude of the modulating signals, the
greater the phase shifts. Assume further that positive alternations of the modulating signal
produce a lagging phase shift and negative signals produce a leading phase shift.
If a constant-amplitude frequency carrier sine wave is applied to the phase shifter, the
output of the phase shifter will be a PM wave. As the modulating signal goes positive, the
amount of phase lag increase with the amplitude modulating signal. This means that the carrier
output is delayed. That delay increases with the amplitude of the modulating signal. The result at
the output is as if the constant-frequency carrier signal had been stretched out or its frequency
lowered.
When the modulating signal goes negative, the phase shift becomes leading. This causes
the carrier sine wave to be effectively speeded up or compressed. The result is as if the carrier
frequency had been increased.
Phase modulation produces frequency modulation. Since the amount of phase shift is
varying, the effect is as is the carrier frequency is changed. Since FM is produced by PM, the
later is often referred to as indirect FM.
It is important to point out that it is the dynamic nature of the modulating that causes the
frequency variation at the output of the phase shifter. In other words, FM is only reduced as long
as the phase shift is being varied.
In FM, maximum deviation occurs at the peak positive and negative amplitudes of the
modulating signal. In PM, the maximum amount of leading ang lagging shift occurs at the peak
amplitude of the modulating signal. The faster the modulating signal voltage varies the greater
the frequency deviation produced. Because of this, the frequency deviation produced in PM
increases with the frequency of the modulating signal. The higher the modulating signal
frequency, naturally the shorter its period and the faster the voltage changes. Higher modulating
voltages produce greater frequency deviation. However, higher modulating frequencies produce
a faster rate of change of modulating voltage and, therefore, also produce greater frequency
deviation.

5. Deviation
When the audio signal is modulated onto the radio frequency carrier, the new radio
frequency signal moves up and down in frequency. The amount by which the signal moves up
and down is important. It is known as the deviation and is normally quoted as the number of
kilohertz deviation. As an example the signal may have a deviation of ±3 kHz. In this case the
carrier is made to move up and down by 3 kHz.
Assume a carrier frequency of 50 MHz .if the peak amplitude of the modulating signal
causes a maximum frequency shift of 200 kHz, the carrier frequency will deviate up to 50.2 MHz
and down to 59.8 MHz. The total frequency deviation is 50.2 – 49.8 = 0.4 MHz = 400 kHz. In
practice, however, the frequency deviation is expressed as the amount of frequency shift of the
carrier above or below the center frequency. Therefore, the frequency deviation in the example
above is said to be 200 kHz. This means that the modulating signal varies the carrier above and
below its center frequency to 200 kHz. The frequency of the modulating signal determines the
rate of frequency deviation but has no effect on the amount of deviation which is strictly a
function of the amplitude of the modulating signal.

6. Advantages of frequency modulation, FM
Although it may not be quite as straightforward as amplitude modulation, nevertheless frequency
modulation, FM, offers some distinct advantages. It is able to provide near interference free
reception, and it was for this reason that it was adopted for the VHF sound broadcasts. These
transmissions could offer high fidelity audio, and for this reason, frequency modulation is far
more popular than the older transmissions on the long, medium and short wave bands.
In addition to its widespread use for high quality audio broadcasts, FM is also sued for a variety
of two way radio communication systems. Whether for fixed or mobile radio communication
systems, or for use in portable applications, FM is widely used at VHF and above.
FM is used for a number of reasons and there are several advantages of frequency modulation. In
view of this it is widely used in a number of areas to which it is ideally suited. Some of the
advantages of frequency modulation are noted below:
Resilience to noise: One particular advantage of frequency modulation is its resilience to
signal level variations. The modulation is carried only as variations in frequency. This
means that any signal level variations will not affect the audio output, provided that the
signal does not fall to a level where the receiver cannot cope. As a result this makes FM
ideal for mobile radio communication applications including more general two-way radio
communication or portable applications where signal levels are likely to vary
considerably. The other advantage of FM is its resilience to noise and interference. It is
for this reason that FM is used for high quality broadcast transmissions.
Easy to apply modulation at a low power stage of the transmitter: Another advantage of
frequency modulation is associated with the transmitters. It is possible to apply the
modulation to a low power stage of the transmitter, and it is not necessary to use a linear
form of amplification to increase the power level of the signal to its final value.
It is possible to use efficient RF amplifiers with frequency modulated signals: It is
possible to use non-linear RF amplifiers to amplify FM signals in a transmitter and these
are more efficient than the linear ones required for signals with any amplitude variations
(e.g. AM and SSB). This means that for a given power output, less battery power is
required and this makes the use of FM more viable for portable two-way radio
applications.

8. Sidebands
Any modulation process produces sidebands. As you saw in AM, when a constant-
frequency sine wave modulates a carrier, two side frequencies are produced. The side
frequencies are the sum and difference of the carrier and the modulating frequency. In FM and
PM too, sum and difference sideband frequencies are produced. In addition, a theoretically
infinite number of pairs of upper and lower sidebands are also generated. As a result, the
spectrum of an FM/PM signal usually wider than an equivalent AM signal. A special
narrowband FM signal whose bandwidth is only slightly wider than that of an AM signal can
also be generated.
Figure 2 shows an example of the spectrum of a typical FM signal produced by
modulating a carrier with a single-frequency sine wave. Note that the sidebands are spaced from
the carrier fc and are space from one another by a frequency equal to the modulating frequency
fm. If the modulating frequency is 500 Hz, the first pair of sidebands are above and below the
carrier by 500 Hz. The second pair of sidebands are above and below the carrier by 2 500 Hz
1000 Hz or 1 kHz, and so on. Note also that the amplitudes/intensities of the sidebands vary. Is
each sideband is assumed to be sine wave with a frequency and amplitude as indicated in Fig 1
and all these sine waves were added together, then the FM signal producing them would be
created.
Figure 2. Frequency Domain Display, fc and sidebands

9. As the amplitude of the modulating signal varies, of course, the frequency deviation will
change. The number of sidebands produced, their amplitude, and their spacing depend upon the
frequency deviation and modulating frequency. Keep in mind that an FM signal has a constant
amplitude. If that FM signal is a summation of the sideband frequencies, then you can see that
the sideband amplitudes must vary with frequency deviation and modulating frequency if their
sum is to produced a fixed amplitude FM signal.
Although the FM process produces an infinite number of upper and lower sidebands, only
those with the largest amplitudes are significant in carrying the information. Typically any
sideband whose amplitude is less than 1 percent of the unmodulated carrier is considered
insignificant. As a result, this markedly narrows the bandwidth of an FM signal.

10. MODULATION INDEX
Modulation Index
As indicated earlier, the number of significant sidebands and their amplitudes are dependent
upon the amount of frequency deviation and the modulating frequency. The ratio so the
frequency deviation to the modulating frequency is known as the modulation index, m.
where fd is the frequency deviation and fm is the modulating frequency.
For example, assume that the maximum frequency deviation of the carrier is 25 kHz while the
maximum modulating frequency is 10 kHz. The modulating index, therefore, is
In most communication systems using FM, maximum limits are put on both the frequency
deviation and the modulating frequency. For example, in standard FM broadcasting, the
maximum permitted frequency deviation is 75 kHz, while the maximum permitted modulating
frequency is 15 kHz. This produce a modulating index of
Whenever the maximum allowable frequency deviation and maximum modulating frequency are
used in computing the modulation index, m is known as the deviation ratio.
Knowing the modulation index, you can compute the number and amplitudes of the significant
sidebands. This is done through a complex mathematical process known as the Bessel function.

11. BESSEL FUNCTION TABLE
Figure 3. the left-hand column gives the modulation index. The remaining columns
indicate the relative amplitudes of the carrier and the various parts of sidebands. Any sideband
with relative carrier amplitude of less than 1 percent has been eliminated. Note that some of the
carrier and sideband amplitudes have negative signs. This means that the signal represented by
the amplitude is simply shifted in phase 180o (phase inversion)
As you can see, the spectrum of an FM signal varies considerably in bandwidth
depending upon the modulation index. The higher the modulation index, the wider the bandwidth
of an FM signals nay be deliberately by putting an upper limit on the modulation index.
Modulation Sideband
index Carrier 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16
0.00 1.00
0.25 0.98 0.12
0.5 0.94 0.24 0.03
1.0 0.77 0.44 0.11 0.02
1.5 0.51 0.56 0.23 0.06 0.01
2.0 0.22 0.58 0.35 0.13 0.03
2.41 0 0.52 0.43 0.20 0.06 0.02
2.5 −0.05 0.50 0.45 0.22 0.07 0.02 0.01
3.0 −0.26 0.34 0.49 0.31 0.13 0.04 0.01
4.0 −0.40 −0.07 0.36 0.43 0.28 0.13 0.05 0.02
5.0 −0.18 −0.33 0.05 0.36 0.39 0.26 0.13 0.05 0.02
5.53 0 −0.34 −0.13 0.25 0.40 0.32 0.19 0.09 0.03 0.01
6.0 0.15 −0.28 −0.24 0.11 0.36 0.36 0.25 0.13 0.06 0.02
7.0 0.30 0.00 −0.30 −0.17 0.16 0.35 0.34 0.23 0.13 0.06 0.02
8.0 0.17 0.23 −0.11 −0.29 −0.10 0.19 0.34 0.32 0.22 0.13 0.06 0.03
8.65 0 0.27 0.06 −0.24 −0.23 0.03 0.26 0.34 0.28 0.18 0.10 0.05 0.02
9.0 −0.09 0.25 0.14 −0.18 −0.27 −0.06 0.20 0.33 0.31 0.21 0.12 0.06 0.03 0.01
10.0 −0.25 0.04 0.25 0.06 −0.22 −0.23 −0.01 0.22 0.32 0.29 0.21 0.12 0.06 0.03 0.01
12.0 0.05 −0.22 −0.08 0.20 0.18 −0.07 −0.24 −0.17 0.05 0.23 0.30 0.27 0.20 0.12 0.07 0.03 0.01
Figure 3 A table showing carrier and sideband amplitudes for different modulation indexes of
FM signals. Based on the Bessel Function.

12. TYPES OF FREQUENCY MODULATION
Wide Band Frequency Modulation – Broadcast stations in the VHF portion of the
frequency spectrum between 88.5 and 108 MHz use large values of deviation, typically ±75 kHz.
This is known as wide-band FM (WBFM). These signals are capable of supporting high quality
transmissions, but occupy a large amount of bandwidth. Usually 200 kHz is allowed for each
wide-band FM transmission.
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).
Narrow Band Frequency Modulation – For communications purposes less bandwidth is
used. Narrow band FM (NBFM) often uses deviation figures of around ±3 kHz. It is narrow band
FM that is typically used for two-way radio communication applications. Having a narrower
band it is not able to provide the high quality of the wideband transmissions, but this is not
needed for applications such as mobile radio communication.
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).
The block diagrams satisfy the corresponding expression for FM.

13. POWER IN FREQUENCY MOULATION
From the equation for FM vs (t ) Vc J n ( ) cos( c n m )t
n
we see that the peak value of the components is VcJn( ) for the nth component.
2
Single normalised average power = V pk 2 then the nth component is
(VRMS )
2
2 2
Vc J n ( ) Vc J n ( )
2 2
Hence, the total power in the infinite spectrum is
Total power (Vc J n ( ))2
PT
n 2
By this method we would need to carry out an infinite number of calculations to find PT. But,
considering the waveform, the peak value is Vc, which is constant.
2
V pk Vc
Since we know that the RMS value of a sine wave is
2 2
2 2
Vc Vc2 Vc J n ( )
2
and power = (VRMS) then we may deduce that PT
2 2 n 2
Hence, if we know Vc for the FM signal, we can find the total power PT for the infinite spectrum
with a simple calculation.
Now consider – if we generate an FM signal, it will contain an infinite number of sidebands.
However, if we wish to transfer this signal, e.g. over a radio or cable, this implies that we require
an infinite bandwidth channel. Even if there was an infinite channel bandwidth it would not all
be allocated to one user. Only a limited bandwidth is available for any particular signal. Thus we
have to make the signal spectrum fit into the available channel bandwidth. We can think of the
signal spectrum as a „train‟ and the channel bandwidth as a tunnel – obviously we make the train
slightly less wider than the tunnel if we can.

14. However, many signals (e.g. FM, square waves, digital signals) contain an infinite number of
components. If we transfer such a signal via a limited channel bandwidth, we will lose some of
the components and the output signal will be distorted. If we put an infinitely wide train through
a tunnel, the train would come out distorted, the question is how much distortion can be
tolerated? Generally speaking, spectral components decrease in amplitude as we move away
from the spectrum „centre‟.
In general distortion may be defined as
Power in total
spectrum- Power in Bandlimite spectrum
d
D
Power in total
spectrum
PT PBL
D
PT
With reference to FM the minimum channel bandwidth required would be just wide enough to
pass the spectrum of significant components. For a bandlimited FM spectrum, let a = the number
of sideband pairs, e.g. for = 5, a = 8 pairs (16 components). Hence, power in the bandlimited
spectrum PBL is
a
(Vc J n ( ))2 = carrier power + sideband powers.
PBL
n a 2

15. Vc2
Since PT
2
Vc2 Vc2 a
( J n ( ))2 a
2 2 n a
Distortion D 1 ( J n ( ))2
Vc2 n a
2
Also, it is easily seen that the ratio
a
Power in Bandlimite spectrum PBL
d
D ( J n ( ))2 = 1 – Distortion
Power in total
spectrum PT n a
a
i.e. proportion pf power in band limited spectrum to total power = ( J n ( ))2
n a