1, producing more than two sidebands. As β increases, more sidebands are produced, increasing the bandwidth. Phase modulation (PM) varies the phase of the carrier signal based on the modulating signal, while frequency modulation (FM) varies the frequency of the carrier. PM has maximum phase deviation at zero crossings of the modulating signal, while FM has maximum frequency deviation at the peaks."> 1, producing more than two sidebands. As β increases, more sidebands are produced, increasing the bandwidth. Phase modulation (PM) varies the phase of the carrier signal based on the modulating signal, while frequency modulation (FM) varies the frequency of the carrier. PM has maximum phase deviation at zero crossings of the modulating signal, while FM has maximum frequency deviation at the peaks.">
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Narrowband and Wideband FM

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Narrowband and Wideband FM

Narrowband FM NBFM

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   1 is referred to as narrowband FM (NBFM) (Note, the bandwidth is


the same as DSBAM).

Wideband FM WBFM

For  > 1 there are more than 2 significant sidebands. As  increases the number of
sidebands increases. This is referred to as wideband FM (WBFM).

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Narrowband FM

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Narrowband FM

The expression for AM and NBFM will be same except 180 degree phase shift at
the lower frequency side.

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Narrowband FM

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WIDEBAND FM
The features of Wideband FM are as follows

•This frequency modulation has infinite bandwidth.

•The modulation index is large, i.e., higher than 1.

•Its spectrum consists of a carrier and infinite number of sidebands, which


are located around it.

•This is used in entertainment broadcasting applications such as FM radio,


TV, etc
•General Expression for single tone Wideband FM:

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WIDEBAND FM
𝑛𝑓𝑖𝑡
 
𝑓𝑖𝑡
  𝑓  𝑜 (𝑡 )=𝑛𝑓 𝑐 +𝑛 𝐴𝑚𝑘𝑓 cos(¿2𝜋 𝑓𝑚𝑡)¿
𝑓  𝑖 ( 𝑡 )=𝑓 𝑐 +𝐴𝑚𝑘𝑓 cos(¿ 2 𝜋 𝑓𝑚𝑡)¿ ⨯𝑛
 

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WIDEBAND FM
𝑠  ( 𝑡 ) = 𝐴𝑐cos(2 𝜋 𝑓 𝑐 𝑡)+ 𝛽sin (2¿𝜋 𝑓𝑚𝑡)¿
Cos(θ)= Re[ej θ]

S(t) is periodic function of time with


fundamental frequency fm, using complex
Fourier series

𝑑  𝑡=𝑑𝑥/2π 𝑓𝑚
𝑑  𝑥=2π 𝑓𝑚𝑑𝑡 7
WIDEBAND FM
Bessel function of first kind order n

Nth coefficient of DFT s(t)

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Phase Modulation

• In the phase modulation, we vary the carrier signal


in accordance with the phase of the modulating
signal or message signal

• If the amplitude of message or modulating signal is


huge then the phase shift will also be greater.

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Phase Modulation

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Mathematical Expression of PM

i  t  = kp m t 
The standard equation of angle modulated wave is

s (t ) = Ac cos( 2f c t  i )
Substitute, ϕi value in the above equation.

s (t ) = Ac cos( 2f c t  kp m t  )
If modulating signal
m(t ) = Am cos( 2fmt )
s (t ) = Ac cos( 2f c t  kp Am cos( 2fmt ))
 =   kp Am
s (t ) = Ac cos( 2f c t   cos( 2fmt ))
Δϕ is phase deviation 11
Average Power of a FM or PM
Wave
• The amplitude A is constant in a phase modulated
or a frequency modulated signal. RF power does
not depend upon the frequency or the phase of the
waveform.
A2
Average power =
2R

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FM and PM
• FM – maximum frequency deviation (change in the carrier freq.) occurs during
the maximum positive and negative peaks (zero slope) of the modulating
signal (freq. deviation is proportional to the amplitude of the modulating
signal)
• PM – the maximum phase deviation occurs during the zero crossings (maximum
slope) of the modulating signal (the freq. deviation is proportional to the slope or
first derivative of the modulating signal)

FM PM
Instantaneous frequency of the carrier is Phase angle of the carrier is varied
varied from its reference value by from its reference value by an
an amount proportional to the amount proportional to the
modulating signal amplitude modulating signal amplitude
Freq. carrier - - - > directly varied Phase carrier - - - > directly varied
Phase carrier - - -> indirectly varied Freq. carrier - - -> indirectly varied
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Relation b/w Frequency and
Phase modulation

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Frequency spectrum for FM

Frequency spectrum for PM

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