Difference between revisions of "Aufgaben:Exercise 2.13: Quadrature Amplitude Modulation"
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===Solution=== | ===Solution=== | ||
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− | '''(1)''' | + | '''(1)''' With the given trigonometric transformations we get: |
:$$s(t) = A_1 \cdot \cos(\omega_{\rm 1} \cdot t)\cdot \cos(\omega_{\rm T} \cdot t) + A_2 \cdot \sin(\omega_{\rm 2} \cdot t)\cdot \sin(\omega_{\rm T} \cdot t) $$ | :$$s(t) = A_1 \cdot \cos(\omega_{\rm 1} \cdot t)\cdot \cos(\omega_{\rm T} \cdot t) + A_2 \cdot \sin(\omega_{\rm 2} \cdot t)\cdot \sin(\omega_{\rm T} \cdot t) $$ | ||
:$$\Rightarrow \hspace{0.3cm}s(t) = \frac{A_1}{2}\cdot \cos((\omega_{\rm T} - \omega_{\rm 1})\cdot t) + \frac{A_1}{2}\cdot \cos((\omega_{\rm T} + \omega_{\rm 1})\cdot t) + | :$$\Rightarrow \hspace{0.3cm}s(t) = \frac{A_1}{2}\cdot \cos((\omega_{\rm T} - \omega_{\rm 1})\cdot t) + \frac{A_1}{2}\cdot \cos((\omega_{\rm T} + \omega_{\rm 1})\cdot t) + | ||
\frac{A_2}{2}\cdot \cos((\omega_{\rm T} - \omega_{\rm 2})\cdot t) - \frac{A_2}{2}\cdot \cos((\omega_{\rm T} + \omega_{\rm 2})\cdot t)\hspace{0.05cm}.$$ | \frac{A_2}{2}\cdot \cos((\omega_{\rm T} - \omega_{\rm 2})\cdot t) - \frac{A_2}{2}\cdot \cos((\omega_{\rm T} + \omega_{\rm 2})\cdot t)\hspace{0.05cm}.$$ | ||
− | * | + | *The <u>second answer</u> is correct. |
− | '''(2)''' | + | '''(2)''' With $A_1 = A_2 = 2 \ \rm V$ and $f_1 = f_2 = 5\ \rm kHz$, the first and third cosine oscillations constructively overlap and the other two cancel completely. |
− | * | + | *Thus, the following simple result is obtained: |
:$$ s(t) = 2\,{\rm V} \cdot \cos(2 \pi \cdot 20\,{\rm kHz} \cdot t) \hspace{0.3cm}\Rightarrow \hspace{0.3cm} s(t = 50\,{\rm µ s}) \hspace{0.15cm}\underline {= 2\,{\rm V}} \hspace{0.05cm}.$$ | :$$ s(t) = 2\,{\rm V} \cdot \cos(2 \pi \cdot 20\,{\rm kHz} \cdot t) \hspace{0.3cm}\Rightarrow \hspace{0.3cm} s(t = 50\,{\rm µ s}) \hspace{0.15cm}\underline {= 2\,{\rm V}} \hspace{0.05cm}.$$ | ||
− | '''(3)''' | + | '''(3)''' The<u>first answer</u> is correct: |
− | * | + | *For phase-synchronous demodulation $(Δϕ_T = 0)$ , the signals before the low-pass filters according to subtask '''(2)''' are obtained as: |
:$$b_1(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \cos(\omega_{\rm 25} \cdot t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 5} \cdot t) + 2\,{\rm V} \cdot \cos(\omega_{\rm 45} \cdot t),$$ | :$$b_1(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \cos(\omega_{\rm 25} \cdot t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 5} \cdot t) + 2\,{\rm V} \cdot \cos(\omega_{\rm 45} \cdot t),$$ | ||
:$$ b_2(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \sin(\omega_{\rm 25} \cdot t) = 2\,{\rm V} \cdot \sin(\omega_{\rm 5} \cdot t) + 2\,{\rm V} \cdot \sin(\omega_{\rm 45} \cdot t)\hspace{0.05cm}.$$ | :$$ b_2(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \sin(\omega_{\rm 25} \cdot t) = 2\,{\rm V} \cdot \sin(\omega_{\rm 5} \cdot t) + 2\,{\rm V} \cdot \sin(\omega_{\rm 45} \cdot t)\hspace{0.05cm}.$$ | ||
− | * | + | *Thus, after eliminating the respective $45\ \rm kHz$ components, we get $v_1(t) = q_1(t)$ and $v_2(t) = q_2(t)$. |
− | '''(4)''' | + | '''(4)''' Analogously to subtask '''(3)''' it now holds that: |
:$$ b_1(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \cos(\omega_{\rm 25} \cdot t+ \Delta \phi_{\rm T})= | :$$ b_1(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \cos(\omega_{\rm 25} \cdot t+ \Delta \phi_{\rm T})= | ||
2\,{\rm V} \cdot \cos(\omega_{\rm 5} \cdot t + \Delta \phi_{\rm T}) + {(45 \,\rm kHz-Anteil )},$$ | 2\,{\rm V} \cdot \cos(\omega_{\rm 5} \cdot t + \Delta \phi_{\rm T}) + {(45 \,\rm kHz-Anteil )},$$ | ||
:$$b_2(t)= 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \sin(\omega_{\rm 25} \cdot t+ \Delta \phi_{\rm T})= | :$$b_2(t)= 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \sin(\omega_{\rm 25} \cdot t+ \Delta \phi_{\rm T})= | ||
2\,{\rm V} \cdot \sin(\omega_{\rm 5} \cdot t + \Delta \phi_{\rm T}) + {(45 \,\rm kHz-Anteil )}\hspace{0.05cm}.$$ | 2\,{\rm V} \cdot \sin(\omega_{\rm 5} \cdot t + \Delta \phi_{\rm T}) + {(45 \,\rm kHz-Anteil )}\hspace{0.05cm}.$$ | ||
− | * | + | *The sink signals $v_1(t)$ and $v_2(t)$ in this constellation exhibit delays and thus phase distortions compared with $q_1(t)$ and $q_2(t)$ . |
− | * | + | *These belong to the class of linear distortions ⇒ <u>Answer 2</u>. |
− | '''(5)''' | + | '''(5)''' In general, it holds for the source signal that: |
:$$r(t) = s(t) = q_1(t) \cdot \cos(\omega_{\rm T} \cdot t) + q_2(t) \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | :$$r(t) = s(t) = q_1(t) \cdot \cos(\omega_{\rm T} \cdot t) + q_2(t) \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$ | ||
− | + | Multiplication by the receiver-side carrier signals $z_{1,\hspace{0.05cm}{\rm E}}(t)$ and $z_{2,\hspace{0.05cm}{\rm E}}(t)$ and band-limiting leads to the signals | |
:$$v_1(t) = \cos(\Delta \phi_{\rm T}) \cdot q_1(t) - \sin(\Delta \phi_{\rm T}) \cdot q_2(t),$$ | :$$v_1(t) = \cos(\Delta \phi_{\rm T}) \cdot q_1(t) - \sin(\Delta \phi_{\rm T}) \cdot q_2(t),$$ | ||
:$$ v_2(t) = \sin(\Delta \phi_{\rm T}) \cdot q_1(t) + \cos(\Delta \phi_{\rm T}) \cdot q_2(t) \hspace{0.05cm}.$$ | :$$ v_2(t) = \sin(\Delta \phi_{\rm T}) \cdot q_1(t) + \cos(\Delta \phi_{\rm T}) \cdot q_2(t) \hspace{0.05cm}.$$ | ||
− | + | From this it can be seen: | |
− | * | + | *With a phase offset of $Δϕ_{\rm T} = 30^\circ$ , the sink signal $v_1(t)$ includes not only the signal $q_1(t)$ attenuated by about $\cos(30^\circ) = 0.866$ , but also the frequency $f_2$ contained in $q_2(t)$ . |
− | * | + | *This is weighted by the factor $\sin(30^\circ) = 0.5$ . |
− | * | + | *Thus, nonlinear distortions are present ⇒ <u>Answer 3</u>. |
{{ML-Fuß}} | {{ML-Fuß}} |
Revision as of 17:25, 23 December 2021
The quadrature amplitude modulation $\rm (QAM)$ explained by the diagram allows the transmission of two source signals $q_1(t)$ and $q_2(t)$ over the same channel, under certain boundary conditions, which are to be determined in this task.
In this exercise, with $A_1 = A_2 = 2\ \rm V$, let:
- $$q_1(t) = A_1 \cdot \cos(2 \pi \cdot f_{\rm 1} \cdot t),$$
- $$q_2(t) = A_2 \cdot \sin(2 \pi \cdot f_{\rm 2} \cdot t)\hspace{0.05cm}.$$
For $ω_{\rm T} = 2π · 25\ \rm kHz$, the four carrier signals shown in the diagram are:
- $$z_1(t) = \cos(\omega_{\rm T} \cdot t),$$
- $$ z_2(t) = \sin(\omega_{\rm T} \cdot t),$$
- $$ z_{1,\hspace{0.05cm}{\rm E}}(t) = 2 \cdot \cos(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T}),$$
- $$ z_{2,\hspace{0.05cm}{\rm E}}(t) = 2 \cdot \sin(\omega_{\rm T} \cdot t + \Delta \phi_{\rm T})\hspace{0.05cm}.$$
Both lowpass filters $\rm TP_1$ and $\rm TP_2$ with input signals $b_1(t)$ and $b_2(t)$ , respectively, remove all frequency components $|f| > f_{\rm T}$.
Hints:
- This exercise belongs to the chapter Further AM Variants.
- Particular reference is made to the page Quadrature Amplitude Modulation (QAM).
- It is worth noting that the carrier signals $z_2(t)$ and $z_{2,\hspace{0.05cm}{\rm E}}(t)$ are applied with positive signs here.
- Often – as in the theory section – these carrier signals are given as "minus-sine".
- The following trigonometric transformations are given:
- $$ \cos(\alpha) \cdot \cos(\beta) = 1/2 \cdot \big[ \cos(\alpha - \beta)+ \cos(\alpha + \beta) \big],$$
- $$ \sin(\alpha) \cdot \sin(\beta) = 1/2 \cdot \big[ \cos(\alpha - \beta)- \cos(\alpha + \beta) \big],$$
- $$ \sin(\alpha) \cdot \cos(\beta) = 1/2 \cdot \big[ \sin(\alpha - \beta)+ \sin(\alpha + \beta) \big] \hspace{0.05cm}.$$
Questions
Solution
- $$s(t) = A_1 \cdot \cos(\omega_{\rm 1} \cdot t)\cdot \cos(\omega_{\rm T} \cdot t) + A_2 \cdot \sin(\omega_{\rm 2} \cdot t)\cdot \sin(\omega_{\rm T} \cdot t) $$
- $$\Rightarrow \hspace{0.3cm}s(t) = \frac{A_1}{2}\cdot \cos((\omega_{\rm T} - \omega_{\rm 1})\cdot t) + \frac{A_1}{2}\cdot \cos((\omega_{\rm T} + \omega_{\rm 1})\cdot t) + \frac{A_2}{2}\cdot \cos((\omega_{\rm T} - \omega_{\rm 2})\cdot t) - \frac{A_2}{2}\cdot \cos((\omega_{\rm T} + \omega_{\rm 2})\cdot t)\hspace{0.05cm}.$$
- The second answer is correct.
(2) With $A_1 = A_2 = 2 \ \rm V$ and $f_1 = f_2 = 5\ \rm kHz$, the first and third cosine oscillations constructively overlap and the other two cancel completely.
- Thus, the following simple result is obtained:
- $$ s(t) = 2\,{\rm V} \cdot \cos(2 \pi \cdot 20\,{\rm kHz} \cdot t) \hspace{0.3cm}\Rightarrow \hspace{0.3cm} s(t = 50\,{\rm µ s}) \hspace{0.15cm}\underline {= 2\,{\rm V}} \hspace{0.05cm}.$$
(3) Thefirst answer is correct:
- For phase-synchronous demodulation $(Δϕ_T = 0)$ , the signals before the low-pass filters according to subtask (2) are obtained as:
- $$b_1(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \cos(\omega_{\rm 25} \cdot t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 5} \cdot t) + 2\,{\rm V} \cdot \cos(\omega_{\rm 45} \cdot t),$$
- $$ b_2(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \sin(\omega_{\rm 25} \cdot t) = 2\,{\rm V} \cdot \sin(\omega_{\rm 5} \cdot t) + 2\,{\rm V} \cdot \sin(\omega_{\rm 45} \cdot t)\hspace{0.05cm}.$$
- Thus, after eliminating the respective $45\ \rm kHz$ components, we get $v_1(t) = q_1(t)$ and $v_2(t) = q_2(t)$.
(4) Analogously to subtask (3) it now holds that:
- $$ b_1(t) = 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \cos(\omega_{\rm 25} \cdot t+ \Delta \phi_{\rm T})= 2\,{\rm V} \cdot \cos(\omega_{\rm 5} \cdot t + \Delta \phi_{\rm T}) + {(45 \,\rm kHz-Anteil )},$$
- $$b_2(t)= 2\,{\rm V} \cdot \cos(\omega_{\rm 20} \cdot t)\cdot 2 \cdot \sin(\omega_{\rm 25} \cdot t+ \Delta \phi_{\rm T})= 2\,{\rm V} \cdot \sin(\omega_{\rm 5} \cdot t + \Delta \phi_{\rm T}) + {(45 \,\rm kHz-Anteil )}\hspace{0.05cm}.$$
- The sink signals $v_1(t)$ and $v_2(t)$ in this constellation exhibit delays and thus phase distortions compared with $q_1(t)$ and $q_2(t)$ .
- These belong to the class of linear distortions ⇒ Answer 2.
(5) In general, it holds for the source signal that:
- $$r(t) = s(t) = q_1(t) \cdot \cos(\omega_{\rm T} \cdot t) + q_2(t) \cdot \sin(\omega_{\rm T} \cdot t) \hspace{0.05cm}.$$
Multiplication by the receiver-side carrier signals $z_{1,\hspace{0.05cm}{\rm E}}(t)$ and $z_{2,\hspace{0.05cm}{\rm E}}(t)$ and band-limiting leads to the signals
- $$v_1(t) = \cos(\Delta \phi_{\rm T}) \cdot q_1(t) - \sin(\Delta \phi_{\rm T}) \cdot q_2(t),$$
- $$ v_2(t) = \sin(\Delta \phi_{\rm T}) \cdot q_1(t) + \cos(\Delta \phi_{\rm T}) \cdot q_2(t) \hspace{0.05cm}.$$
From this it can be seen:
- With a phase offset of $Δϕ_{\rm T} = 30^\circ$ , the sink signal $v_1(t)$ includes not only the signal $q_1(t)$ attenuated by about $\cos(30^\circ) = 0.866$ , but also the frequency $f_2$ contained in $q_2(t)$ .
- This is weighted by the factor $\sin(30^\circ) = 0.5$ .
- Thus, nonlinear distortions are present ⇒ Answer 3.