Exercise 3.5: PM and FM for Rectangular Signals
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)=AT⋅cos[ψ(t)]
Here, we distinguish between phase modulation (PM) with the angular function
- ψ(t)=ωT⋅t+ϕ(t)=ωT⋅t+KPM⋅q(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+KFM⋅q(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:
- This exercise belongs to the chapter Frequency Modulation.
- Reference is also made to the chapter Phase Modulation.
- 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
Solution
- 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}.