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TELE3113 Analogue and Digital
      Communications
                Angle Modulation

                      Wei Zhang
                 w.zhang@unsw.edu.au


School of Electrical Engineering and Telecommunications
          The University of New South Wales
Last two weeks ...
We have studied:
    Amplitude Modulation:
       s(t) = [1 + ka m(t)]c(t).
       Simple envelope detection, but low power/BW efficiency.
    DSB-SC Modulation:
       s(t) = m(t)c(t).
       High power efficiency, but low BW efficiency.
    SSB Modulation:
    s(t) = 1 Ac m(t) cos(2πfc t)
           2
                                   1
                                   2 Ac m(t) sin(2πfc t).
                                        ˆ
    VSB Modulation: Tailored for transmission of TV signals.
                                                    TELE3113 - Angle Modulation. August 18, 2009. – p.1/1
Angle vs Amplitude Modulation

 Amplitude modulation: amplitude of a carrier wave varies in
 accordance with an information-bearing signal.
 Angle modulation: angle of the carrier changes according to
 the information-bearing signal.
 Angle modulation provides better robustness to noise and
 interference than amplitude modulation, but at the cost of
 increased transmission BW.




                                           TELE3113 - Angle Modulation. August 18, 2009. – p.2/1
Definitions

 Let θi (t) denote the angle of a modulated sinusoidal carrier
 at time t.
 Assume θi (t) is a function of the information-bearing signal
 or message signal m(t).
 The angle-modulated wave is

                      s(t) = Ac cos[θi (t)]

 Instantaneous frequency of s(t) is defined as

                                 1 dθi (t)
                       fi (t) =
                                2π dt

                                              TELE3113 - Angle Modulation. August 18, 2009. – p.3/1
PM
Two commonly used angle modulation: PM and FM.
   Phase modulation (PM): The instantaneous angle is varied
   linearly with m(t), as shown by

                     θi (t) = 2πfc t + kp m(t),

   where kp denotes the phase-sensitivity factor.
   The phase-modulated wave is described by

                  s(t) = Ac cos[2πfc t + kp m(t)].




                                                  TELE3113 - Angle Modulation. August 18, 2009. – p.4/1
FM

 Frequency modulation (FM): The instantaneous frequency
 fi (t) is varied linearly with m(t), as shown by

                              fi (t) = fc + kf m(t),

 where kf denotes the frequency-sensitivity factor.
 Integrating fi (t) with time and multiplying 2π, we get
                       t                                       t
     θi (t) = 2π           fi (τ )dτ = 2πfc t + 2πkf               m(τ )dτ.                       (1)
                   0                                       0

 The frequency-modulated wave is therefore
                                                      t
           s(t) = Ac cos 2πfc t + 2πkf                    m(τ )dτ .
                                                  0            TELE3113 - Angle Modulation. August 18, 2009. – p.5/1
PM versus FM

         Phase Modulation           Frequency Modulation


                                                    t
θi (t)   2πfc t + kp m(t)           2πfc t + 2πkf   0 m(τ )dτ


                kp d
fi (t)   fc +   2π dt m(t)          fc + kf m(t)


                                                                    t
s(t)     Ac cos[2πfc t + kp m(t)]   Ac cos 2πfc t + 2πkf            0 m(τ )dτ




                                                     TELE3113 - Angle Modulation. August 18, 2009. – p.6/1
PM/FM Relationship

    Modulating
      wave                                   Phase             FM wave
                    Integrator              modulator




                                           Ac cos( 2πf c t )

      (a) Scheme for generating an FM wave by using a phase modulator.




    Modulating
      wave                                  Frequency          PM wave
                   Differentiator           modulator




                                           Ac cos( 2πf c t )

    (b) Scheme for generating a PM wave by using a frequency modulator.
                                                               TELE3113 - Angle Modulation. August 18, 2009. – p.7/1
AM/PM/FM Waves
                  Carrier Wave
   1

   0

  −1
       0   0.5   Message Signal   1                       1.5
   1

   0

  −1
       0   0.5     AM Wave        1                       1.5
   2

   0

  −2
       0   0.5     PM Wave        1                       1.5
   1

   0

  −1
       0   0.5     FM Wave        1                       1.5
   1

   0

  −1
       0   0.5                    1                      1.5
                                      TELE3113 - Angle Modulation. August 18, 2009. – p.8/1
Properties of Angle Modulation

 Property 1 Constancy of transmitted power:
 The average power of angle-modulated waves is a constant,
 as shown by
                                    1 2
                              Pav = Ac .
                                    2
 Property 2 Nonlinearity of the modulation process:
 Let s(t), s1 (t), and s2 (t) denote the PM waves produced by
 m(t), m1 (t) and m2 (t). If m(t) = m1 (t) + m2 (t), then

                     s(t) = s1 (t) + s2 (t).




                                               TELE3113 - Angle Modulation. August 18, 2009. – p.9/1
Properties of Angle Modulation

 Property 3 Irregularity of zero-crossings:
 A “zero-crossing” is a point where the sign of a function
 changes. PM and FM wave no longer have a perfect
 regularity in their spacing across the time-scale.
 Property 4 Visualization difficulty of message
 waveform:
 The message waveform cannot be visualized from PM and
 FM waves.




                                             TELE3113 - Angle Modulation. August 18, 2009. – p.10/1
Example of Zero-crossings (1)

Consider a modulating wave m(t) as shown by
                           
                            at, t ≥ 0
                    m(t) =
                            0, t < 0

Determine the zero-crossings of the PM and FM waves produced
by m(t) with carrier frequency fc and carrier amplitude Ac .




                                              TELE3113 - Angle Modulation. August 18, 2009. – p.11/1
Example of Zero-crossings (2)
The PM wave is given by
                  
                   A cos(2πf t + k at), t ≥ 0
                       c      c     p
          s(t) =
                   Ac cos(2πfc t),      t<0

The PM wave experiences a zero-crossing when the angle is an
odd multiple of π/2, i.e.,
                            π
          2πfc tn + kp atn = + nπ,        n = 0, 1, 2, · · ·
                            2
Then, we get

                      1/2 + n
               tn =              ,   n = 0, 1, 2, · · ·
                    2fc + kp a/π
                                                     TELE3113 - Angle Modulation. August 18, 2009. – p.12/1
Example of Zero-crossings (3)
The FM wave is given by
                 
                  A cos(2πf t + πk at2 ), t ≥ 0
                      c      c     f
          s(t) =
                  Ac cos(2πfc t),         t<0

To find zero-crossings, we may set up
                               π
          2πfc tn + πkf at2
                          n   = + nπ,   n = 0, 1, 2, · · ·
                               2
The positive root of the above quadratic equation is

         1               2
                                     1
   tn =        −fc +    fc   + akf     +n    ,   n = 0, 1, 2, · · ·
        akf                          2

                                                 TELE3113 - Angle Modulation. August 18, 2009. – p.13/1
Example of Zero-crossings (4)

fc = 0.25, a = 1, kp = π/2 and kf = 1.
                           Message Signal
            8

            6

            4

            2

            0
            −8   −6   −4   −2      0      2   4      6            8
                                PM Wave
            1

           0.5

            0

          −0.5

           −1
            −8   −6   −4   −2      0      2   4      6            8
                                FM Wave
            1

           0.5

            0

          −0.5

           −1
            −8   −6   −4   −2      0      2   4      6            8

                                                  TELE3113 - Angle Modulation. August 18, 2009. – p.14/1
Narrowband FM (1)

 Consider a sinusoidal modulating wave defined by

                     m(t) = Am cos(2πfm t).

 The instantaneous frequency of the FM wave is

     fi (t) = fc + kf Am cos(2πfm t) = fc + ∆f cos(2πfm t)

 where ∆f = kf Am is called the frequency deviation.
 The angle of the FM wave is

                   θi (t) = 2πfc t + β sin(2πfm t)
             ∆f
 where β =   fm   is called the modulation index of the FM
 wave.                                          TELE3113 - Angle Modulation. August 18, 2009. – p.15/1
Narrowband FM (2)
The FM wave is then given by

                s(t) = Ac cos[2πfc t + β sin(2πfm t)].

Using cos(x + y) = cos x cos y − sin x sin y, we get

s(t) = Ac cos(2πfc t) cos[β sin(2πfm t)]−Ac sin(2πfc t) sin[β sin(2πfm t)].

For narrowband FM wave, β << 1. Then, cos[β sin(2πfm t)] ≈ 1
and sin[β sin(2πfm t)] ≈ β sin(2πfm t). Therefore,

        s(t) ≈ Ac cos(2πfc t) − βAc sin(2πfc t) sin(2πfm t).



                                                   TELE3113 - Angle Modulation. August 18, 2009. – p.16/1
Generating Narrowband FM

Modulating                                        __
  wave                                                                        Narrow-
                                Product
             Integrator                                     ∑                  band
                               Modulator                                      FM wave

                                        Ac sin( 2πf c t )         +

                                  − 90 0
                               Phase-shifter


                    Narrow-band phase
                        modulator
                                                   Carrier wave
                                                 Ac cos(2πf c t )



                                                            TELE3113 - Angle Modulation. August 18, 2009. – p.17/1
Narrowband FM vs. AM
For small β, the narrowband FM wave is given by

        s(t) ≈ Ac cos(2πfc t) − βAc sin(2πfc t) sin(2πfm t).

Using sin x sin y = − 1 cos(x + y) cos(x − y), we get
                      2

                       1
s(t) ≈ Ac cos(2πfc t) + βAc [cos[2π(fc + fm )t] − cos[2π(fc − fm )t]].
                       2
Recall the AM of the single-tone message signal is [p.11, Aug-4,
TELE3113]
                         1
sAM (t) = Ac cos(2πfc t)+ µAc [cos[2π(fc +fm )t]+cos[2π(fc −fm )t]].
                         2

The only difference between NB-FM and AM is the “sign”.
                                                   TELE3113 - Angle Modulation. August 18, 2009. – p.18/1

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Tele3113 wk5tue

  • 1. TELE3113 Analogue and Digital Communications Angle Modulation Wei Zhang w.zhang@unsw.edu.au School of Electrical Engineering and Telecommunications The University of New South Wales
  • 2. Last two weeks ... We have studied: Amplitude Modulation: s(t) = [1 + ka m(t)]c(t). Simple envelope detection, but low power/BW efficiency. DSB-SC Modulation: s(t) = m(t)c(t). High power efficiency, but low BW efficiency. SSB Modulation: s(t) = 1 Ac m(t) cos(2πfc t) 2 1 2 Ac m(t) sin(2πfc t). ˆ VSB Modulation: Tailored for transmission of TV signals. TELE3113 - Angle Modulation. August 18, 2009. – p.1/1
  • 3. Angle vs Amplitude Modulation Amplitude modulation: amplitude of a carrier wave varies in accordance with an information-bearing signal. Angle modulation: angle of the carrier changes according to the information-bearing signal. Angle modulation provides better robustness to noise and interference than amplitude modulation, but at the cost of increased transmission BW. TELE3113 - Angle Modulation. August 18, 2009. – p.2/1
  • 4. Definitions Let θi (t) denote the angle of a modulated sinusoidal carrier at time t. Assume θi (t) is a function of the information-bearing signal or message signal m(t). The angle-modulated wave is s(t) = Ac cos[θi (t)] Instantaneous frequency of s(t) is defined as 1 dθi (t) fi (t) = 2π dt TELE3113 - Angle Modulation. August 18, 2009. – p.3/1
  • 5. PM Two commonly used angle modulation: PM and FM. Phase modulation (PM): The instantaneous angle is varied linearly with m(t), as shown by θi (t) = 2πfc t + kp m(t), where kp denotes the phase-sensitivity factor. The phase-modulated wave is described by s(t) = Ac cos[2πfc t + kp m(t)]. TELE3113 - Angle Modulation. August 18, 2009. – p.4/1
  • 6. FM Frequency modulation (FM): The instantaneous frequency fi (t) is varied linearly with m(t), as shown by fi (t) = fc + kf m(t), where kf denotes the frequency-sensitivity factor. Integrating fi (t) with time and multiplying 2π, we get t t θi (t) = 2π fi (τ )dτ = 2πfc t + 2πkf m(τ )dτ. (1) 0 0 The frequency-modulated wave is therefore t s(t) = Ac cos 2πfc t + 2πkf m(τ )dτ . 0 TELE3113 - Angle Modulation. August 18, 2009. – p.5/1
  • 7. PM versus FM Phase Modulation Frequency Modulation t θi (t) 2πfc t + kp m(t) 2πfc t + 2πkf 0 m(τ )dτ kp d fi (t) fc + 2π dt m(t) fc + kf m(t) t s(t) Ac cos[2πfc t + kp m(t)] Ac cos 2πfc t + 2πkf 0 m(τ )dτ TELE3113 - Angle Modulation. August 18, 2009. – p.6/1
  • 8. PM/FM Relationship Modulating wave Phase FM wave Integrator modulator Ac cos( 2πf c t ) (a) Scheme for generating an FM wave by using a phase modulator. Modulating wave Frequency PM wave Differentiator modulator Ac cos( 2πf c t ) (b) Scheme for generating a PM wave by using a frequency modulator. TELE3113 - Angle Modulation. August 18, 2009. – p.7/1
  • 9. AM/PM/FM Waves Carrier Wave 1 0 −1 0 0.5 Message Signal 1 1.5 1 0 −1 0 0.5 AM Wave 1 1.5 2 0 −2 0 0.5 PM Wave 1 1.5 1 0 −1 0 0.5 FM Wave 1 1.5 1 0 −1 0 0.5 1 1.5 TELE3113 - Angle Modulation. August 18, 2009. – p.8/1
  • 10. Properties of Angle Modulation Property 1 Constancy of transmitted power: The average power of angle-modulated waves is a constant, as shown by 1 2 Pav = Ac . 2 Property 2 Nonlinearity of the modulation process: Let s(t), s1 (t), and s2 (t) denote the PM waves produced by m(t), m1 (t) and m2 (t). If m(t) = m1 (t) + m2 (t), then s(t) = s1 (t) + s2 (t). TELE3113 - Angle Modulation. August 18, 2009. – p.9/1
  • 11. Properties of Angle Modulation Property 3 Irregularity of zero-crossings: A “zero-crossing” is a point where the sign of a function changes. PM and FM wave no longer have a perfect regularity in their spacing across the time-scale. Property 4 Visualization difficulty of message waveform: The message waveform cannot be visualized from PM and FM waves. TELE3113 - Angle Modulation. August 18, 2009. – p.10/1
  • 12. Example of Zero-crossings (1) Consider a modulating wave m(t) as shown by   at, t ≥ 0 m(t) =  0, t < 0 Determine the zero-crossings of the PM and FM waves produced by m(t) with carrier frequency fc and carrier amplitude Ac . TELE3113 - Angle Modulation. August 18, 2009. – p.11/1
  • 13. Example of Zero-crossings (2) The PM wave is given by   A cos(2πf t + k at), t ≥ 0 c c p s(t) =  Ac cos(2πfc t), t<0 The PM wave experiences a zero-crossing when the angle is an odd multiple of π/2, i.e., π 2πfc tn + kp atn = + nπ, n = 0, 1, 2, · · · 2 Then, we get 1/2 + n tn = , n = 0, 1, 2, · · · 2fc + kp a/π TELE3113 - Angle Modulation. August 18, 2009. – p.12/1
  • 14. Example of Zero-crossings (3) The FM wave is given by   A cos(2πf t + πk at2 ), t ≥ 0 c c f s(t) =  Ac cos(2πfc t), t<0 To find zero-crossings, we may set up π 2πfc tn + πkf at2 n = + nπ, n = 0, 1, 2, · · · 2 The positive root of the above quadratic equation is 1 2 1 tn = −fc + fc + akf +n , n = 0, 1, 2, · · · akf 2 TELE3113 - Angle Modulation. August 18, 2009. – p.13/1
  • 15. Example of Zero-crossings (4) fc = 0.25, a = 1, kp = π/2 and kf = 1. Message Signal 8 6 4 2 0 −8 −6 −4 −2 0 2 4 6 8 PM Wave 1 0.5 0 −0.5 −1 −8 −6 −4 −2 0 2 4 6 8 FM Wave 1 0.5 0 −0.5 −1 −8 −6 −4 −2 0 2 4 6 8 TELE3113 - Angle Modulation. August 18, 2009. – p.14/1
  • 16. Narrowband FM (1) Consider a sinusoidal modulating wave defined by m(t) = Am cos(2πfm t). The instantaneous frequency of the FM wave is fi (t) = fc + kf Am cos(2πfm t) = fc + ∆f cos(2πfm t) where ∆f = kf Am is called the frequency deviation. The angle of the FM wave is θi (t) = 2πfc t + β sin(2πfm t) ∆f where β = fm is called the modulation index of the FM wave. TELE3113 - Angle Modulation. August 18, 2009. – p.15/1
  • 17. Narrowband FM (2) The FM wave is then given by s(t) = Ac cos[2πfc t + β sin(2πfm t)]. Using cos(x + y) = cos x cos y − sin x sin y, we get s(t) = Ac cos(2πfc t) cos[β sin(2πfm t)]−Ac sin(2πfc t) sin[β sin(2πfm t)]. For narrowband FM wave, β << 1. Then, cos[β sin(2πfm t)] ≈ 1 and sin[β sin(2πfm t)] ≈ β sin(2πfm t). Therefore, s(t) ≈ Ac cos(2πfc t) − βAc sin(2πfc t) sin(2πfm t). TELE3113 - Angle Modulation. August 18, 2009. – p.16/1
  • 18. Generating Narrowband FM Modulating __ wave Narrow- Product Integrator ∑ band Modulator FM wave Ac sin( 2πf c t ) + − 90 0 Phase-shifter Narrow-band phase modulator Carrier wave Ac cos(2πf c t ) TELE3113 - Angle Modulation. August 18, 2009. – p.17/1
  • 19. Narrowband FM vs. AM For small β, the narrowband FM wave is given by s(t) ≈ Ac cos(2πfc t) − βAc sin(2πfc t) sin(2πfm t). Using sin x sin y = − 1 cos(x + y) cos(x − y), we get 2 1 s(t) ≈ Ac cos(2πfc t) + βAc [cos[2π(fc + fm )t] − cos[2π(fc − fm )t]]. 2 Recall the AM of the single-tone message signal is [p.11, Aug-4, TELE3113] 1 sAM (t) = Ac cos(2πfc t)+ µAc [cos[2π(fc +fm )t]+cos[2π(fc −fm )t]]. 2 The only difference between NB-FM and AM is the “sign”. TELE3113 - Angle Modulation. August 18, 2009. – p.18/1