Exercise 2.9: Symmetrical Distortions
The source signal made up of two components
- q(t)=A1⋅cos(2πf1t)+A2⋅cos(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:
- This exercise belongs to the chapter Envelope Demodulation.
- Particular reference is made to the section Description using the equivalent low-pass signal.
Questions
Solution
- {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 .