Principles of Communication system
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Module-2
Mrs. Bhavya S and Dr Rashmi Samanth
Senior Assistant Professor, ECE,
MITE-Moodbidri
Principles of Communication system
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Outline
Module-2
Angle Modulation
Let carrier signal is represented as
s (t) = Ac cos ϴ(t)
Here phase angle is varied by the message signal m(t).
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Angle Modulation
Note that in this type of modulation the amplitude of signal carries information.
Here the amplitude Ac remains constant and the angle is modulated.
This Modulation Technique is called the Angle Modulation
Angle modulation: Vary either the Phase or the Frequency of the carrier signal
Angle Modulation
Representation of PM and FM signals:
The Complex Envelope for an Angle Modulation is given by
Is a constant Real envelope,
θ(t) - linear function of the modulating signal m(t)
The Angle-modulated Signal in time domain is given by
g(t) - Nonlinear function of the modulation.
Special Case 1:
For PM the phase is directly proportional to the modulating signal. i.e.;
Where Dp is the Phase sensitivity of the phase modulator, having units of radians/volt.
Special Case 2:
For FM, the phase is proportional to the integral of m(t) so that
where the frequency deviation constant Df has units of radians/volt-sec.
Angle Modulation
Resulting PM wave:
Dp is the phase sensitivity of the modulator
Resulting FM wave:
Df is the frequency deviation constant
Phase and Frequency Modulations
Comparing above two equations , we see that if we have a PM signal modulated by mp(t), there is also FM on the signal, corresponding to a different modulation wave shape that is given by:
Similarly if we have a FM signal modulated by mf(t),the corresponding phase modulation on this signal is:
Where f and p denote frequency and phase respectively.
Integrator
Phase Modulator (Carrier Frequency fc)
Differentiator
Frequency Modulator (Carrier Frequency fc)
Generation of FM from PM and vice versa
FM Signal
PM signal
Generation of FM using a Phase Modulator:
Generation of PM using a Frequency Modulator:
FM with sinusoidal modulating signal
∆F is related to the peak modulating voltage by
Where
If a bandpass signal is represented by:
FM with sinusoidal modulating signal
But,
🡺
Vp
BW
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🡺
Average Power does not change with modulation
Angle Modulation
Advantages:
Disadvantages:
Modulation Index
∆θ is related to the peak modulating voltage by:
Where
Where ∆θ is the peak phase deviation
∆F Peak Frequency Deviation
B Bandwidth of the modulating signal
Spectra of Angle modulated signals
Where
Spectrum of Angle modulated signal
Spectrum of PM or FM Signal with Sinusoidal Modulating Signal
Then
Where is the phase Modulation Index.
Same θ(t) could also be obtained if FM were used
where
The Complex Envelope is:
and
The peak frequency deviation would be
which is periodic with period
Using discrete Fourier series that is valid over all time, g(t) can be written as
Where
Which reduces to
Jn(β) – Bessel function of the first kind of the nth order
Taking the fourier transform of the complex envelope g(t), we get
Is a special property of Bessel Functions
Spectrum of PM or FM Signal with Sinusoidal Modulating Signal
or
Bessel Functions of the First Kind
J0(β)=0 at β=2.4, 5.52 & so on
Bessel Functions of the First Kind
Observations:
Frequency spectrum of FM
Spectra of an FM Signal with Sinusoidal Modulation
BT
f
1.0
BT
J0(1.0)
J1(1.0)
J2(1.0)
f
1.0
Spectra of an FM Signal with Sinusoidal Modulation
BT
f
1.0
Spectra of an FM Signal with Sinusoidal Modulation
Carson’s rule
(1+β)fm
Carson’s rule
β – phase modulation index/ frequency modulation index
B – bandwidth of the modulating signal
For sinusoidal modulation
Note: When β =0 i.e. baseband signals
Narrowband Angle Modulation
becomes
where
PM
FM
Indirect method of generating WBFM
Balanced Modulator
Wideband Frequency modulation
FM Stero System
FM Stero System
Phase–Locked Loop
Phase–Locked Loop
Phase–Locked Loop
Phase–Locked Loop
Phase–Locked Loop- Linear model
Phase–Locked Loop- Linear model
Phase–Locked Loop- Linear model
Phase–Locked Loop- Linear model
The Superheterodyne Receiver �
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