The diagram on the right shows
- the spectrum Gs(f) of the basic transmission pulse,
- the frequency response HE(f) of the receiver filter
of a binary and bipolar transmission system, which are identical in shape to each other:
- Gs(f)={A⋅cos(π⋅f2⋅f2)0for|f|≤f2,else,
- HE(f)={1⋅cos(π⋅f2⋅f2)0for|f|≤f2,else.
In the whole exercise A = 10^{–6} \ \rm V/Hz and f_{2} = 1 \ \rm MHz are valid.
- Assuming that the bit rate R = 1/T is chosen correctly, the basic transmitter pulse g_{d}(t) = g_{s}(t) ∗ h_{\rm E}(t) satisfies the first Nyquist criterion.
- For the associated spectral function G_{d}(f), the rolloff thereby occurs cosinusoidally similar to a cosine rolloff spectrum.
- The rolloff factor r is to be determined in this exercise.
Notes:
- The exercise belongs to the chapter "Optimization of Baseband Transmission Systems".
- Numerical values of the Q-function are provided, for example, by the interactive HTML5/JS applet "Complementary Gaussian Error Functions".
- The crest factor is the quotient of the maximum and the rms value of the transmitted signal and thus a measure of the intersymbol interfering at the transmitting end:
- C_{\rm S} = \frac{s_0}{\sqrt{E_{\rm B}/T}} = \frac{{\rm Max}[s(t)]}{\sqrt{{\rm E}[s^2(t)]}}= {s_0}/{s_{\rm eff}}.
Questions
Solution
(1) With the functions G_{s}(f) and H_{\rm E}(f), the spectrum of the basic detection pulse for |f| \leq f_{2}:
- G_d(f) = G_s(f) \cdot H_{\rm E}(f) = A \cdot \cos^2 \left( \frac {\pi \cdot f}{2 \cdot f_2} \right).
- According to the general definition of the cosine rolloff spectrum, the corner frequencies are f_{1} = 0 and f_{2} = 1\ \rm MHz.
- From this follows for the Nyquist frequency (symmetry point with respect to the rolloff):
- f_{\rm Nyq} = \frac{f_1 +f_2 } {2 } \hspace{0.1cm}\underline { = 0.5\,{\rm MHz}}\hspace{0.05cm}.
- The rolloff factor is
- r = \frac{f_2 -f_1 } {f_2 +f_1 } \hspace{0.1cm}\underline {= 1} \hspace{0.05cm}.
- This means: G_{d}(f) describes a \cos^{2} spectrum.
(2) The relationship between Nyquist frequency and symbol duration T is f_{\rm Nyq} = 1/(2T).
- From this it follows for the bit rate R = 1/T = 2 \cdot f_{\rm Nyq}\ \underline{= 1 \ \rm Mbit/s}.
- Note the different units for frequency and bit rate.
(3) The first and third solutions are correct:
- This is an optimal binary system under the constraint of power limitation.
- The crest factor is not important under power limitation. With the conditions given here, C_{\rm S} > 1 would apply.
(4) The bit error probability of an optimal system can be calculated as follows:
- p_{\rm B} = {\rm Q} \left( \sqrt{{2 \cdot E_{\rm B}}/{N_0}}\right)\hspace{0.05cm}.
- In the given example, we obtain for the average energy per bit:
- E_{\rm B} = \ \int_{-\infty}^{+\infty}|G_s(f)|^2 \,{\rm d} f = A^2 \cdot \int_{-1/T}^{+1/T} H_{\rm Nyq}(f) \,{\rm d} f = \ \frac {A^2}{T} = \frac {(10^{-6}\,{\rm V/Hz})^2}{10^{-6}\,{\rm s}} = 10^{-6}\,{\rm V^2s}\hspace{0.05cm}.
- With N_{0} = 8 \cdot 10^{–8} \ \rm V^{2}/Hz, this further gives:
- p_{\rm B} = {\rm Q} \left( \sqrt{\frac{2 \cdot 10^{-6}\,{\rm V^2s}}{8 \cdot 10^{-8}\,{\rm V^2/Hz}}}\right)= {\rm Q} \left( \sqrt{25}\right)= {\rm Q} (5) \hspace{0.1cm}\underline {= 0.287 \cdot 10^{-6}}\hspace{0.05cm}.