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Exercise 2.9: Symmetrical Distortions

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Transmitter and receiver spectrum in the equivalent low-pass region

The source signal made up of two components

q(t)=A1cos(2πf1t)+A2cos(2πf2t)

is amplitude modulated and transmitted through a linearly distorting transmission channel. 

  • The carrier frequency is  fT  and the added DC component  AT
  • Thus,  a  "double-sideband amplitude moduluation"  \rm (DSB–AM) with carrier"  is present.


The upper graph shows the spectrum  S_{\rm TP}(f)  of the equivalent low-pass signal in schematic form.  This means that the lengths of the Dirac lines drawn do not correspond to the actual values of  A_{\rm T},  A_1/2  and  A_2/2.


The spectral function  R(f)  of the received signal was measured.  In the lower graph we can observe the equivalent low-pass spectrum  R_{\rm TP}(f) calculated from this.

The channel frequency response is characterized with sufficient accuracy with a few auxiliary values:

H_{\rm K}(f = f_{\rm T}) = 0.5,
H_{\rm K}(f = f_{\rm T} \pm f_1) = 0.4,
H_{\rm K}(f = f_{\rm T} \pm f_2) = 0.2 \hspace{0.05cm}.



Hints:


Questions

1

Give the amplitudes of the carrier and source signal.

A_{\rm T} \ = \hspace{0.17cm}

\ \rm V
A_1 \ = \

\ \rm V
A_2 \ = \

\ \rm V

2

Which kind of distortion would the application of an envelope demodulator in an ideal channel   ⇒   H_{\rm K}(f) = 1  lead to?

No distortion.
Linear distortions.
Nonlinear distortions.

3

Calculate the equivalent low-pass signal and answer the following questions. Is it true that...

r_{\rm TP}(t)  is always real,
r_{\rm TP}(t)  is always greater than or equal to zero,
the phase function  ϕ(t)  can take on the values  0^\circ  and  180^\circ .

4

Which kind of distortion does the envelope demodulator in the observed transmission channel lead to?

No distortion.
Linear distortions.
Nonlinear distortions.


Solution

(1)  On the basis of the graphs on the exercise page, the following statements can be made:

{A_{\rm T}} \cdot 0.5 = 2 \,{\rm V}\hspace{0.3cm} \Rightarrow \hspace{0.3cm}A_{\rm T} \hspace{0.15cm}\underline {= 4 \,{\rm V}},
{A_{\rm 1}}/{2} \cdot 0.4 = 0.6\,{\rm V}\hspace{0.3cm} \Rightarrow \hspace{0.3cm}A_{\rm 1} \hspace{0.15cm}\underline {= 3 \,{\rm V}},
{A_{\rm 2}}/{2} \cdot 0.2 = 0.4\,{\rm V}\hspace{0.3cm} \Rightarrow \hspace{0.3cm}A_{\rm 2} \hspace{0.15cm}\underline {= 4 \,{\rm V}}\hspace{0.05cm}.


(2)  Answer 3 is correct:

  • The resulting modulation depth is   m = (A_1 + A_2)/A_T = 1.75.
  • This leads to strong nonlinear distortion when using an envelope demodulator.
  • A distortion factor cannot be specified because the source signal contains two frequency components.



(3)  Answers 1 and 2 are correct:

  • The Fourier retransform of   R_{\rm TP}(f)  gives us the result:
r_{\rm TP}(t) = 2 \,{\rm V} + 1.2 \,{\rm V} \cdot \cos(2 \pi f_1 t ) + 0.8 \,{\rm V} \cdot \cos(2 \pi f_2 t )\hspace{0.05cm}.
  • This function is always real and non-negative.
  • Thus,   ϕ(t) = 0.  holds simultaneously, whereas  ϕ(t) = 180^\circ  is not possible.



(4)  A comparison of the two signals

q(t) = 3 \,{\rm V} \cdot \cos(2 \pi f_1 t ) + 4 \,{\rm V} \cdot \cos(2 \pi f_2 t ),
v(t) = 0.4 \cdot 3 \,{\rm V} \cdot \cos(2 \pi f_1 t ) + 0.2 \cdot 4 \,{\rm V} \cdot \cos(2 \pi f_2 t )
shows, that linear distortions now arise – attenuation distortions to be precise   ⇒   Answer 2.
  • Here, the channel  H_{\rm K}(f)  has the positive effect, that instead of irreversible nonlinear distortions, only linear distortions arise, and these can be eliminated by a downstream filter.
  • This is due to the fact that the higher attenuation of the source signal  q(t)  compared to the carrier signal  z(t)  lowers the modulation depth from   m = 1.75  to  m = (0.4 · 3 \ \rm V + 0.2 · 4 \ \rm V)/(0.5 · 4 \ \rm V) = 1 .