Difference between revisions of "Aufgaben:Exercise 4.6Z: Locality Curve for Phase Modulation"
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− | {{quiz-Header|Buchseite=Signal_Representation/ | + | {{quiz-Header|Buchseite=Signal_Representation/Equivalent Low-Pass Signal and its Spectral Function |
}} | }} | ||
− | [[File:P_ID768__Sig_Z_4_6.png|right|frame| | + | [[File:P_ID768__Sig_Z_4_6.png|right|frame|A possible locality curve with phase modulation]] |
− | + | We assume a source signal q(t), which is considered normalised. | |
− | * | + | *The maximum value of this signal is qmax=1 and the minimum signal value is qmin=−0.5. |
− | * | + | *Otherwise nothing is known about q(t). |
− | + | The modulated signal with phase modulation ⇒ "transmission signal" is: | |
:s(t)=s0⋅cos(ωTt+η⋅q(t)). | :s(t)=s0⋅cos(ωTt+η⋅q(t)). | ||
− | + | Here η denotes the so-called "modulation index". Let the constant envelope s0 also be a normalise quantity, which is set to s0=2 in the following (see diagram). | |
− | + | If one replaces the cosine function with the complex exponential function, one arrives at the analytical signal | |
:$$s_{\rm +}(t) = s_0\cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm}( | :$$s_{\rm +}(t) = s_0\cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm}( | ||
\omega_{\rm T} \hspace{0.05cm}\cdot \hspace{0.05cm} t + \eta \hspace{0.05cm} \cdot \hspace{0.05cm} q(t)) }.$$ | \omega_{\rm T} \hspace{0.05cm}\cdot \hspace{0.05cm} t + \eta \hspace{0.05cm} \cdot \hspace{0.05cm} q(t)) }.$$ | ||
− | + | From this, one can calculate the equivalent low-pass signal sketched in the graph as follows: | |
:$$s_{\rm TP}(t) = s_{\rm +}(t) \cdot {\rm e}^{-{\rm | :$$s_{\rm TP}(t) = s_{\rm +}(t) \cdot {\rm e}^{-{\rm | ||
j}\hspace{0.05cm} \cdot\hspace{0.05cm} \omega_{\rm T} \hspace{0.05cm}\cdot\hspace{0.05cm} t } = s_0\cdot | j}\hspace{0.05cm} \cdot\hspace{0.05cm} \omega_{\rm T} \hspace{0.05cm}\cdot\hspace{0.05cm} t } = s_0\cdot | ||
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+ | ''Hints:'' | ||
+ | *This exercise belongs to the chapter [[Signal_Representation/Equivalent_Low-Pass_Signal_and_its_Spectral_Function|Equivalent Low-Pass Signal and its Spectral Function]]. | ||
+ | |||
+ | *You can check your solution with the interactive applet [[Applets:Physical_Signal_%26_Equivalent_Lowpass_Signal|Physical Signal & Equivalent Low-Pass Signal]] ⇒ "Locality Curve". | ||
− | |||
− | |||
− | |||
− | |||
− | === | + | ===Questions=== |
<quiz display=simple> | <quiz display=simple> | ||
− | { | + | {What is the magnitude function a(t)=|sTP(t)|? Which value is valid for t=0? |
|type="{}"} | |type="{}"} | ||
a(t=0) = { 2 3% } | a(t=0) = { 2 3% } | ||
− | { | + | {Between which extreme values ϕmin and ϕmax does the phase ϕ(t)? |
|type="{}"} | |type="{}"} | ||
− | ϕmin = { -93--87 } $\text{ | + | ϕmin = { -93--87 } $\text{deg}$ |
− | ϕmin = { 180 3% } $\text{ | + | ϕmin = { 180 3% } $\text{deg}$ |
− | { | + | {Determine the modulation index η from the phase function ϕ(t). |
|type="{}"} | |type="{}"} | ||
η = { 3.1415 3% } | η = { 3.1415 3% } | ||
− | { | + | {Which of the following statements are true? |
|type="[]"} | |type="[]"} | ||
− | - | + | - From q(t)=−0.5=const. follows s(t)=s0⋅cos(ωT⋅t). |
− | + | + | + With a rectangular signal (with only two possible signal values $q(t)=\pm 0.5)$ the locality curve degenerates to two points. |
− | + | + | + With the signal values ±1 (qmin=−0.5 is then no longer valid) the locality curve degenerates to one point: sTP(t)=−s0. |
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</quiz> | </quiz> | ||
− | === | + | ===Solution=== |
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' | + | '''(1)''' The locality curve is a circular arc with radius 2. Therefore, the magnitude function is constant a(t)=2_. |
− | '''(2)''' | + | '''(2)''' From the graph it can be seen that the following numerical values apply: |
*ϕmin=−π/2⇒−90∘_, | *ϕmin=−π/2⇒−90∘_, | ||
*ϕmax=+π⇒+180∘_. | *ϕmax=+π⇒+180∘_. | ||
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− | '''(3)''' | + | '''(3)''' In general, the relation $s_{\rm TP}(t) = a(t) \cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm} |
− | \phi(t)}. | + | \phi(t)}$ applies here. A comparison with the given function yields: |
:ϕ(t)=η⋅q(t). | :ϕ(t)=η⋅q(t). | ||
− | * | + | *The maximum phase value ϕmax=+π⇒180∘ is obtained for the signal amplitude qmax=1. From this follows directly ${\eta = \pi} \; \underline{\approx 3.1415}$. |
− | * | + | *This modulation index is confirmed by the values ϕmin=−π/2 and qmin=−0.5 . |
− | [[File:P_ID769__Sig_Z_4_6_d_neu.png|right|frame| | + | [[File:P_ID769__Sig_Z_4_6_d_neu.png|right|frame|Locality curve (phase diagram) for a rectangular source signal]] |
− | '''(4)''' | + | '''(4)''' <u>The second and third proposed solutions</u> are correct: |
− | * | + | *If q(t)=const.=−0.5, the phase function is also constant: |
:$$\phi(t) = \eta \cdot q(t) = - {\pi}/{2}\hspace{0.3cm} | :$$\phi(t) = \eta \cdot q(t) = - {\pi}/{2}\hspace{0.3cm} | ||
\Rightarrow \hspace{0.3cm} s_{\rm TP}(t) = - {\rm j} \cdot s_0 = - 2{\rm j}.$$ | \Rightarrow \hspace{0.3cm} s_{\rm TP}(t) = - {\rm j} \cdot s_0 = - 2{\rm j}.$$ | ||
− | * | + | *Thus, for the actual physical signal: |
:$$s(t) = s_0 \cdot {\cos} ( \omega_{\rm T}\hspace{0.05cm} t - | :$$s(t) = s_0 \cdot {\cos} ( \omega_{\rm T}\hspace{0.05cm} t - | ||
{\pi}/{2}) = 2 \cdot {\sin} ( \omega_{\rm T} \hspace{0.05cm} t ).$$ | {\pi}/{2}) = 2 \cdot {\sin} ( \omega_{\rm T} \hspace{0.05cm} t ).$$ | ||
− | * | + | *In contrast, q(t)=+0.5 leads to ϕ(t)=π/2 and to sTP(t)=2j. |
− | * | + | *If q(t) is a rectangular signal that alternates between +0.5 and –0.5 , then the locality curve consists of only two points on the imaginary axis, regardless of how long the intervals with +0.5 and –0.5 last. |
− | * | + | *If, on the other hand, q(t)=±1, then the possible phase values +π and −π result purely formally, but they are identical. |
− | * | + | *The locality curve then consists of only one point: sTP(t)=−s0 ⇒ the signal s(t) is "minus-cosine" for all times t. |
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__NOEDITSECTION__ | __NOEDITSECTION__ | ||
− | [[Category: | + | [[Category:Signal Representation: Exercises|^4.3 Equivalent LP Signal and its Spectral Function^]] |
Latest revision as of 15:02, 24 May 2021
We assume a source signal q(t), which is considered normalised.
- The maximum value of this signal is qmax=1 and the minimum signal value is qmin=−0.5.
- Otherwise nothing is known about q(t).
The modulated signal with phase modulation ⇒ "transmission signal" is:
- s(t)=s0⋅cos(ωTt+η⋅q(t)).
Here η denotes the so-called "modulation index". Let the constant envelope s0 also be a normalise quantity, which is set to s0=2 in the following (see diagram).
If one replaces the cosine function with the complex exponential function, one arrives at the analytical signal
- s+(t)=s0⋅ej⋅(ωT⋅t+η⋅q(t)).
From this, one can calculate the equivalent low-pass signal sketched in the graph as follows:
- sTP(t)=s+(t)⋅e−j⋅ωT⋅t=s0⋅ej⋅η⋅q(t).
Hints:
- This exercise belongs to the chapter Equivalent Low-Pass Signal and its Spectral Function.
- You can check your solution with the interactive applet Physical Signal & Equivalent Low-Pass Signal ⇒ "Locality Curve".
Questions
Solution
(2) From the graph it can be seen that the following numerical values apply:
- ϕmin=−π/2⇒−90∘_,
- ϕmax=+π⇒+180∘_.
(3) In general, the relation sTP(t)=a(t)⋅ej⋅ϕ(t) applies here. A comparison with the given function yields:
- ϕ(t)=η⋅q(t).
- The maximum phase value ϕmax=+π⇒180∘ is obtained for the signal amplitude qmax=1. From this follows directly η=π≈3.1415_.
- This modulation index is confirmed by the values ϕmin=−π/2 and qmin=−0.5 .
(4) The second and third proposed solutions are correct:
- If q(t)=const.=−0.5, the phase function is also constant:
- ϕ(t)=η⋅q(t)=−π/2⇒sTP(t)=−j⋅s0=−2j.
- Thus, for the actual physical signal:
- s(t)=s0⋅cos(ωTt−π/2)=2⋅sin(ωTt).
- In contrast, q(t)=+0.5 leads to ϕ(t)=π/2 and to sTP(t)=2j.
- If q(t) is a rectangular signal that alternates between +0.5 and –0.5 , then the locality curve consists of only two points on the imaginary axis, regardless of how long the intervals with +0.5 and –0.5 last.
- If, on the other hand, q(t)=±1, then the possible phase values +π and −π result purely formally, but they are identical.
- The locality curve then consists of only one point: sTP(t)=−s0 ⇒ the signal s(t) is "minus-cosine" for all times t.