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Exercise 3.5: PM and FM for Rectangular Signals

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Zwei Signalverläufe bei Winkelmodulation

Assume a bipolar and rectangular source signal q(t) , as shown in the upper diagram.  This signal can only take on the two signal values  ±A=±2 V  and the duration of the positive and negative rectangles are each T=1 ms.  The period of  q(t)  is therefore  T0=2 ms.

The signals s1(t)  and  s2(t)  display two transmit signals with angle modulation  (WM), each of which can be represented as

s(t)=ATcos[ψ(t)]

Here, we distinguish between phase modulation  (PM)  with the angular function

ψ(t)=ωTt+ϕ(t)=ωTt+KPMq(t)

and frequency modulation  (FM), where the instantaneous freqiency is linearly related to q(t):

fA(t)=ωA(t)2π,ωA(t)=dψ(t)dt=ωT+KFMq(t).

KPM  and  KFM  denote the dimensionally constrained constants given by the realizations of the PM and FM modulators, respectively.  The frequency deviation  Δf_{\rm A}  indicates the maximum deviation of the instantaneous frequency from the carrier frequency.





Hints:

  • In anticipation of the fourth chapter, it should be mentioned that phase modulation with a digital input signal is also called Phase Shift Keying  \rm (PSK)  and frequency modulation is analogously called Frequency Shift Keying  \rm (FSK) .


Questions

1

Which of the signals is due to phase modulation and which is due to frquency modulation?

s_1(t)  represents a phase modulation.
s_1(t)  represents a frequency modulation.

2

What is the carrier phase  ϕ_{\rm T} that could be measured without a message signal   ⇒   q(t) \equiv 0 ?

ϕ_{\rm T} \ = \

\ \rm Grad

3

What carrier frequency  (with respect to  1/T)  was used in the graphs?

f_{\rm T} · T \ = \

4

The phase of the PM signal is  ±90^\circ.  What is the modulator constant?

K_{\rm PM} \ = \

\ \rm V^{-1}

5

What is the frequency deviation  Δf_{\rm A}  of the FM signal with respect to  1/T?

Δf_{\rm A} · T \ = \

6

What is the FM modulator constant?

K_{\rm FM} \ = \

\ \rm (Vs)^{-1}


Solution

(1)  Answer 2 is correct:

  • For a rectangular (digital) source signal, phase modulation (PM) can be recognised by the typical phase jumps – see the signal waveform  s_2(t).
  • Frequency modulation (FM), on the other hand, has diverse instantaneous frequencies at different times, as in  s_1(t).


(2)  When  q(t) = 0 , the equations provided for both PM and FM give

s(t) = A_{\rm T} \cdot \cos (\omega_{\rm T} \cdot t ) \hspace{0.3cm}\Rightarrow\hspace{0.3cm} \phi_{\rm T} \hspace{0.15cm}\underline {= 0}\hspace{0.05cm}.


(3)  The carrier frequency  f_{\rm T}  can be directly determined only from the PM signal   s_2(t) .

  • By counting the oscillations of  s_2(t)  in the time interval  T , it can be seen that  f_{\rm T} · T\hspace{0.15cm}\underline{ = 6}  was used.
  • When frequency modulating a bipolar source signal,   f_{\rm T}  does not occur directly.
  • However, the graphs do indicate that   f_{\rm T} · T = 6  is also used here.



(4)  The amplitude value  A = 2 \ \rm V  results in the phase  90^\circ  or  π/2  (minus sine wave).  This gives:

K_{\rm PM} = \frac {\pi /2}{2\,{\rm V}} \hspace{0.15cm}\underline {= 0.785\,{\rm V}^{-1}} \hspace{0.05cm}.


(5)  The graph for  s_1(t)  shows that either four or eight oscillations arise within a time interval  T :   4 \le f_{\rm A}(t) \cdot T \le 8\hspace{0.05cm}.

  • Considering the (normalized) carrier frequency  f_{\rm T} · T = 6 , the (normalized) frequency deviation is:
\Delta f_{\rm A} \cdot T \hspace{0.15cm}\underline {=2}\hspace{0.05cm}.


(6)  The frequency deviation can also be represented as follows:

\Delta f_{\rm A} = \frac {K_{\rm FM}}{2\pi}\cdot A \hspace{0.05cm}.
  • With   Δf_{\rm A} · {\rm A} = 2  we thus get:
K_{\rm FM} = \frac {2 \cdot 2\pi}{A \cdot T}= \frac {4\pi}{2\,{\rm V} \cdot 1\,{\rm ms}}\hspace{0.15cm}\underline {= 6283 \,{\rm V}^{-1}{\rm s}^{-1}} \hspace{0.05cm}.