Difference between revisions of "Aufgaben:Exercise 5.2Z: About PN Modulation"
From LNTwww
m (Textersetzung - „*Sollte die Eingabe des Zahlenwertes „0” erforderlich sein, so geben Sie bitte „0.” ein.“ durch „ “) |
|||
(15 intermediate revisions by 3 users not shown) | |||
Line 1: | Line 1: | ||
− | {{quiz-Header|Buchseite= | + | {{quiz-Header|Buchseite=Modulation_Methods/Direct-Sequence_Spread_Spectrum_Modulation |
}} | }} | ||
− | [[File: | + | [[File:EN_Bei_A_4_5.png|right|frame|Models of PN modulation (top) and BPSK (bottom)]] |
− | + | The upper diagram shows the equivalent circuit of PN modulation $($Direct-Sequence Spread Spectrum, abbreviated $\rm DS–SS)$ in the equivalent low-pass range, based on AWGN noise n(t). | |
− | + | Shown below is the low-pass model of binary phase shift keying \rm (BPSK). | |
+ | *The low-pass transmitted signal s(t) is set equal to the rectangular source signal q(t) ∈ \{+1, –1\} with rectangular duration T for reasons of uniformity. | ||
+ | |||
+ | *The function of the integrator can be described as follows: | ||
:d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t \hspace{0.05cm}. | :d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t \hspace{0.05cm}. | ||
− | + | *The two models differ by multiplication with the ±1 spreading signal c(t) at transmitter and receiver, where only the spreading factor J is known from c(t). | |
− | + | ||
+ | It has to be investigated whether the lower BPSK model can also be used for PN modulation and whether the BPSK error probability | ||
:p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt { {2 \cdot E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right ) | :p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt { {2 \cdot E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right ) | ||
− | + | is also valid for PN modulation, or how the given equation should be modified. | |
+ | |||
+ | |||
+ | |||
+ | |||
+ | Notes: | ||
+ | *This exercise belongs to the chapter [[Modulation_Methods/Direct-Sequence_Spread_Spectrum_Modulation|Direct-Sequence Spread Spectrum Modulation]]. | ||
− | + | *For the solution of this exercise, the specification of the specific spreading sequence $(M-sequence or Walsh function)$ is not important. | |
− | * | ||
− | |||
− | === | + | ===Questions=== |
<quiz display=simple> | <quiz display=simple> | ||
− | { | + | {Which detection signal values are possible with BPSK (in the noise-free case)? |
|type="[]"} | |type="[]"} | ||
− | - d(νT) | + | - d(νT) can be Gaussian distributed. |
− | - d(νT) | + | - d(νT) can take the values +1, 0 and -1. |
− | + | + | + Only the values d(νT) = +1 and d(νT) = -1 are possible. |
− | { | + | {Which values are possible in PN modulation (in the noise-free) case? |
|type="[]"} | |type="[]"} | ||
− | - d(νT) | + | - d(νT) can be Gaussian distributed. |
− | - d(νT) | + | - d(νT) can take the values +1, 0 and -1. |
− | + | + | + Only the values d(νT) = +1 and d(νT) = -1 are possible. |
− | { | + | {What modification must be made to the BPSK model to make it applicable to PN modulation? |
|type="[]"} | |type="[]"} | ||
− | + | + | + The noise n(t) must be replaced by n'(t) = n(t) · c(t). |
− | - | + | - The integration must now be done over J · T. |
− | - | + | - The noise power σ_n^2 must be reduced by a factor of J. |
− | { | + | {What is the bit error probability $p_{\rm B}$ for 10 \lg \ (E_{\rm B}/N_0) = 6\ \rm dB for PN modulation? <br>Note: For BPSK, the following applies in this case: p_{\rm B} ≈ 2.3 · 10^{–3}. |
− | <br> | + | |type="()"} |
− | |type=" | + | - The larger J is chosen, the smaller p_{\rm B} is. |
− | - | + | - The larger J is chosen, the larger p_{\rm B} is. |
− | - | + | + Independent of J, the value p_{\rm B} ≈ 2.3 · 10^{–3} is always obtained. |
− | + | ||
</quiz> | </quiz> | ||
− | === | + | ===Solution=== |
{{ML-Kopf}} | {{ML-Kopf}} | ||
− | '''(1)''' | + | '''(1)''' The <u>last solution</u> is correct: |
− | * | + | *We are dealing here with an optimal receiver. |
− | * | + | *Without noise, the signal b(t) within each bit is constantly equal to +1 or -1. |
+ | *From the given equation for the integrator | ||
:d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t | :d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t | ||
− | : | + | :it follows that d(νT) can take only the values +1 and -1. |
+ | |||
+ | |||
+ | |||
+ | '''(2)''' Again the <u>last solution</u> is correct: | ||
+ | * In the noise-free and interference-free case ⇒ n(t) = 0, the twofold multiplication by c(t) ∈ \{+1, –1\} can be omitted, | ||
+ | *so that the upper model is identical to the lower model. | ||
− | |||
− | |||
+ | '''(3)''' <u>Solution 1</u> is correct: | ||
+ | *Since both models are identical in the noise-free case, only the noise signal has to be adjusted: n'(t) = n(t) · c(t). | ||
+ | *In contrast, the other two solutions are not applicable: | ||
+ | *The integration must still be done over T = J · T_c and the PN modulation does not reduce the AWGN noise. | ||
− | |||
− | |||
− | |||
− | '''(4)''' | + | '''(4)''' The <u>last solution</u> is correct: |
− | * | + | *Multiplying the AWGN noise by the high-frequency ±1 signal c(t), the product is also Gaussian and white. |
− | * | + | *Because of ${\rm E}\big[c^2(t)\big] = 1$, the noise variance is not changed either. Thus: |
− | * | + | *The equation p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt {{2 E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right ) valid for BPSK is also applicable for PN modulation, independent of spreading factor J and specific spreading sequence. |
− | *Ergo: | + | *Ergo: For AWGN noise, band spreading neither increases nor decreases the error probability. |
{{ML-Fuß}} | {{ML-Fuß}} | ||
− | [[Category: | + | [[Category:Modulation Methods: Exercises|^5.2 PN Modulation^]] |
Latest revision as of 18:55, 4 March 2023
The upper diagram shows the equivalent circuit of \rm PN modulation (Direct-Sequence Spread Spectrum, abbreviated \rm DS–SS) in the equivalent low-pass range, based on AWGN noise n(t).
Shown below is the low-pass model of binary phase shift keying \rm (BPSK).
- The low-pass transmitted signal s(t) is set equal to the rectangular source signal q(t) ∈ \{+1, –1\} with rectangular duration T for reasons of uniformity.
- The function of the integrator can be described as follows:
- d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t \hspace{0.05cm}.
- The two models differ by multiplication with the ±1 spreading signal c(t) at transmitter and receiver, where only the spreading factor J is known from c(t).
It has to be investigated whether the lower BPSK model can also be used for PN modulation and whether the BPSK error probability
- p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt { {2 \cdot E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right )
is also valid for PN modulation, or how the given equation should be modified.
Notes:
- This exercise belongs to the chapter Direct-Sequence Spread Spectrum Modulation.
- For the solution of this exercise, the specification of the specific spreading sequence (M-sequence or Walsh function) is not important.
Questions
Solution
(1) The last solution is correct:
- We are dealing here with an optimal receiver.
- Without noise, the signal b(t) within each bit is constantly equal to +1 or -1.
- From the given equation for the integrator
- d (\nu T) = \frac{1}{T} \cdot \hspace{-0.1cm} \int_{(\nu -1 )T }^{\nu T} \hspace{-0.3cm} b (t )\hspace{0.1cm} {\rm d}t
- it follows that d(νT) can take only the values +1 and -1.
(2) Again the last solution is correct:
- In the noise-free and interference-free case ⇒ n(t) = 0, the twofold multiplication by c(t) ∈ \{+1, –1\} can be omitted,
- so that the upper model is identical to the lower model.
(3) Solution 1 is correct:
- Since both models are identical in the noise-free case, only the noise signal has to be adjusted: n'(t) = n(t) · c(t).
- In contrast, the other two solutions are not applicable:
- The integration must still be done over T = J · T_c and the PN modulation does not reduce the AWGN noise.
(4) The last solution is correct:
- Multiplying the AWGN noise by the high-frequency ±1 signal c(t), the product is also Gaussian and white.
- Because of {\rm E}\big[c^2(t)\big] = 1, the noise variance is not changed either. Thus:
- The equation p_{\rm B} = {\rm Q} \left( \hspace{-0.05cm} \sqrt {{2 E_{\rm B}}/{N_{\rm 0}} } \hspace{0.05cm} \right ) valid for BPSK is also applicable for PN modulation, independent of spreading factor J and specific spreading sequence.
- Ergo: For AWGN noise, band spreading neither increases nor decreases the error probability.