Difference between revisions of "Aufgaben:Exercise 3.5: PM and FM for Rectangular Signals"
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− | {{quiz-Header|Buchseite= | + | {{quiz-Header|Buchseite=Modulation_Methods/Frequency_Modulation_(FM) |
}} | }} | ||
− | [[File:P_ID1099__Mod_A_3_5.png|right|frame| | + | [[File:P_ID1099__Mod_A_3_5.png|right|frame|Two signal waveforms in angle modulation]] |
− | + | 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 transmitted signals with angle modulation $\rm (WM)$, each of which can be represented as | |
− | + | :$$s(t) = A_{\rm T} \cdot \cos \hspace{-0.05cm}\big [\psi (t) \big ]$$ | |
− | + | Here, we distinguish between phase modulation $\rm (PM)$ with the angular function | |
− | :$$s(t) = A_{\rm T} \cdot \cos | ||
− | |||
:ψ(t)=ωT⋅t+ϕ(t)=ωT⋅t+KPM⋅q(t) | :ψ(t)=ωT⋅t+ϕ(t)=ωT⋅t+KPM⋅q(t) | ||
− | + | and frequency modulation $\rm (FM)$, where the instantaneous freqiency is linearly related to q(t): | |
:fA(t)=ωA(t)2π,ωA(t)=dψ(t)dt=ωT+KFM⋅q(t). | :fA(t)=ωA(t)2π,ωA(t)=dψ(t)dt=ωT+KFM⋅q(t). | ||
− | KPM | + | K_{\rm PM} and K_{\rm FM} 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. |
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− | '' | + | ''Hints:'' |
− | * | + | *This exercise belongs to the chapter [[Modulation_Methods/Frequency_Modulation_(FM)|Frequency Modulation]]. |
− | * | + | *Reference is also made to the chapter [[Modulation_Methods/Phase_Modulation_(PM)|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=== |
<quiz display=simple> | <quiz display=simple> | ||
− | { | + | {Which of the signals is due to phase modulation and which is due to frquency modulation? |
− | |type=" | + | |type="()"} |
− | - s_1(t) | + | - s_1(t) represents a phase modulation. |
− | + s_1(t) | + | + s_1(t) represents a frequency modulation. |
− | { | + | {What is the carrier phase ϕ_{\rm T} that could be measured without a message signal ⇒ $q(t) \equiv 0$ ? |
|type="{}"} | |type="{}"} | ||
ϕ_{\rm T} \ = \ { 0. } \ \rm Grad | ϕ_{\rm T} \ = \ { 0. } \ \rm Grad | ||
− | { | + | {What carrier frequency $($with respect to $1/T)$ was used in the graphs? |
|type="{}"} | |type="{}"} | ||
f_{\rm T} · T \ = \ { 6 3% } | f_{\rm T} · T \ = \ { 6 3% } | ||
− | { | + | {The phase of the PM signal is ±90^\circ. What is the modulator constant? |
|type="{}"} | |type="{}"} | ||
K_{\rm PM} \ = \ { 0.785 3% } \ \rm V^{-1} | K_{\rm PM} \ = \ { 0.785 3% } \ \rm V^{-1} | ||
− | { | + | {What is the frequency deviation Δf_{\rm A} of the FM signal with respect to 1/T? |
|type="{}"} | |type="{}"} | ||
Δf_{\rm A} · T \ = \ { 2 3% } | Δf_{\rm A} · T \ = \ { 2 3% } | ||
− | { | + | {What is the FM modulator constant? |
|type="{}"} | |type="{}"} | ||
K_{\rm FM} \ = \ { 6283 3% } \ \rm (Vs)^{-1} | K_{\rm FM} \ = \ { 6283 3% } \ \rm (Vs)^{-1} | ||
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</quiz> | </quiz> | ||
− | === | + | ===Solution=== |
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' | + | '''(1)''' <u>Answer 2</u> 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)''' | + | |
+ | '''(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}. | :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}. | ||
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− | |||
− | |||
− | '''(4)''' | + | '''(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}. | :K_{\rm PM} = \frac {\pi /2}{2\,{\rm V}} \hspace{0.15cm}\underline {= 0.785\,{\rm V}^{-1}} \hspace{0.05cm}. | ||
− | '''(5)''' | + | |
− | + | '''(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}. | :\Delta f_{\rm A} \cdot T \hspace{0.15cm}\underline {=2}\hspace{0.05cm}. | ||
− | '''(6)''' | + | |
− | \Delta f_{\rm A} = \frac {K_{\rm FM}}{2\pi}\cdot A \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}. | :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}. | ||
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− | [[Category: | + | [[Category:Modulation Methods: Exercises|^3.2 Frequency Modulation^]] |
Latest revision as of 17:19, 23 January 2023
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 \ \rm V and the duration of the positive and negative rectangles are each T = 1 \ \rm ms. The period of q(t) is therefore T_0 = 2 \ \rm ms.
The signals s_1(t) and s_2(t) display two transmitted signals with angle modulation \rm (WM), each of which can be represented as
- s(t) = A_{\rm T} \cdot \cos \hspace{-0.05cm}\big [\psi (t) \big ]
Here, we distinguish between phase modulation \rm (PM) with the angular function
- \psi(t) = \omega_{\rm T} \cdot t + \phi(t) = \omega_{\rm T} \cdot t + K_{\rm PM} \cdot q(t)
and frequency modulation \rm (FM), where the instantaneous freqiency is linearly related to q(t):
- f_{\rm A}(t) = \frac{\omega_{\rm A}(t)}{2\pi}, \hspace{0.3cm} \omega_{\rm A}(t) = \frac{{\rm d}\hspace{0.03cm}\psi(t)}{{\rm d}t}= \omega_{\rm T} + K_{\rm FM} \cdot q(t)\hspace{0.05cm}.
K_{\rm PM} and K_{\rm FM} 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}.